A t5\L 0 0 - International Nuclear Information System (INIS)

169
INlS-mf—12585 A t5 \L 0 0 LABELLING OF OLIVE OIL WITH RADIOACTIVE IODINE AND RADIOACTIVE TECHNETIUM By OMAR A. F. AL-DAYEL This Dissertation has been examined and accepted for M.Sc. degree on 1st. March 1988- Supervisors: Name Signature Supervisor : prof. H. A. El-Garhy C -supervisor: soc. Prof. A. A. Al-Suhybani Committe members: Name Signature Prof. M. A. El-Garhy M- Asoc. Prof. S. H. Al-Khowaiter : Prof. M. E. Abdullah

Transcript of A t5\L 0 0 - International Nuclear Information System (INIS)

INlS-mf—12585 A t5\L 0 0

LABELLING OF OLIVE OIL WITH RADIOACTIVE IODINE

AND RADIOACTIVE TECHNETIUM

By

OMAR A. F. AL-DAYEL

This Dissertation has been examined and accepted for M.Sc. degreeon 1st. March 1988-

Supervisors:

Name Signature

Supervisor :

prof. H. A. El-Garhy

C-supervisor:

soc. Prof. A. A. Al-Suhybani

Committe members:

Name Signature

Prof. M. A. El-Garhy M-

Asoc. Prof. S. H. Al-Khowaiter :

Prof. M. E. Abdullah

LABELLING OF OLIVE OIL WITH RADIOACTIVE IODINE

AND RADIOACTIVE TECHNETIUH

THIS DISSERTATION IS SUBMITTED IN PARTIAL FULFILMENT OF

THE REQUIREMENTS FOR THE MASTER'S DEGREE IN THE DEPARTMENT OF

CHEMISTRY AT THE COLLEGE OF SCIENCE, KING SAUD UNIVERSITY.(1988)

D E D I C A T I O N :

To my parents, my wife, and my son.

ACKNOWLEDGEMENTS

I wish to acknowedge the generous guidance, advice and help that Ireceived from Professor M. El-Garhy, and Associate Professor Abdulaziz A.Alsuhaibani, who also supervised my research.

I would also like to thank the head of the department and members ofthe staff of Chemistry Department, College of Science, King SaudUniversity.

I am also indebted to. my brother Dr. Mohammed, who helped me andconsistently during the writing of this thesis.

I appreciate the consistent support from all the members of theDirectorate of Atomic Energy, King Abdulaziz City for Science andTechnology (KACST), especially the head of the departmentDr. Abdulrahman Melibary for his valuable advices.

I give special thanks to the Nuclear Medicine department in King

Khalid University Hospital for their help in providing the Tc used inthis work.

I wish to acknowledge the vital role of the Directorate of InformationSystems and Technical Services, King Abdulaziz City for Science andTechnology (KACST) in providing me quickly and precisely the neededreferences.

C O N T E N T S

Page

List of Tables ... ••• ••• i

List of Figures ... .... ... ;;J

Aimz of this work ... ... ... v

Summary ... ... ... ... Vl

CHAPTER 1 : GENERAL INTRODUCTION

1.1 Genera 1 ... ... . . 2

1.2 A r t i f i c i a l Radioisotopes . . . . . . . 5

1.2.A.a. Reactor Produced Isotopes . . . . . . 6

1.2.A.b. Some Theori t ical Aspects of Radioisotope Production 9

1.2.A.C Practical Aspects of Reactor Irradiat ions . . . 12

I.2.B. Accelerator Produced Radioisotopes . . . 13

I.2.C. Radioisotope Generator Systems . . . 15

1.3 Methods of Labelling of Organic Compoundswith Radioactive Iodine Isotopes . . . 18

1.*» 0 1 i v e 0 i 1 . . . . . . 2k

1.5 Historical Cascade of Radioactive Iodine FattyAcids Labelling . . . . . . 27

1.6 Iodine Isotopes and Labelled Compounds . . . 33

CHAPTER 2 : EXPERIMENTAL AND RESULTS

2.1 The iodine Monochloride Method . . . . . . kl

Page

2.2 Label l ing of Oil wi th Inact ive IodineMonochloride Method kk

2.3 Label l ing of Oil with Radioactive Iodine

Monochloride Method . . . 51

2.4 Labell ing of Oil with Chloramine-T Method . . . 59

2.5 Quali ty Control Systems . . . . . . 59

CHAPTER 3 : DISCUSSION AND CONCLUSIONS

3.1 Label 1 ing of 01ive Oil and 01iec Acid w i thIodine Monochloride Method . . . 78

3-2 Label l ing of Olive Oil and 01iec Acid withChloramine-T Method . . . 82

CHAPTER 4 : LABELLING OF OIL WITH 99 lTc

4.1 Introduction ... ... ... 86

4.1.1 Generator Fundamentals ... ... 86

'••I.2 Technetium-99m Milking System . 93

A.1.3 Methods for Separation of ""Vc ... 96

4.1.4 Comparison of Tc Generator Forms ... 97

4.1.5 Use of 99mTc in Labelling ... ... 101

4.2 Experimental and Results ... 103

4.2.1 Preparation and Control of 9mTc ... 104

4.2.2 Determination of Radiocontaminants in Old

99mTc Generators ... 110

4.2.3 Quality Control by Thin Layer Chromatographyand Paper Chromatography ... ... 120

Page

k.2.k Labelling of Olive Oil by " m T c 138

*».2.5 Labelling of Olive Oil by Reduced9 9 m T c 138

R E F E R E N C E S ... ... T»3

L I S T OF TABLES

T A B L E Paae

1. Nuclear Data for Iodine Radionuciides Used

in Nuclear Medicine ... . k

2. Some Common Radioactive Milking Pairs ... 17

3. Methods of Labelling ... ... 22-23

h. Olive Oil Components ... ... 2k

5. Relative Weight of Olive Oil Expressed asPercentage Body Weights of Rats Fed with01ive Oil ... ... 25

6. Principal Fatty Acids of Myocardium of RatsFed with Olive Oil . . . . . . 26

7. Examples of Compounds Labelled with lodine-125and Their Application(s) . . . 35"36

8. Reactions Realized by the Use of an i??Accelerator (Production of |) 37

9. Reactions Realized by the Use of an

Accelerator (Production of 1 2 5 l ) . . . 38-39

10. Reactions Realized in a Nuclear Reactor

(Productionof 1 3 1 | ) kO

1 1 . The U l t r a V i o l e t Spectrum Stud ies f o rL a b e l l i n g O l i ve O i l . . . . . kB-hS

12. Distribution Coefficient of IC1Between Aquous Layer and Organic Layer 52

13- Wave Lengths of Maximum Absorption inDifferent Solvents ... ... 57

I I

Page

1^-16 Th in- layer Chromatography Results 66-68

17. Change of A c t i v i t i e s w i th Time in Aloo mci

^9Mo Generator . . . . . . . 88

18. Nuclear Data f o r Technetium . . . 90

19. Radioactive Isotopes Produced on I r r a d i a t i n gStable Molybdenum in Nuclear Reactor 9*t

20. Compounds Label led by " m T c . . . 102

2 1 . Standard L ib ra ry (Option) . . . 106

22-2A The Radiocontaminants of Old Molybdenum-

Technetium Generators ... 111-113

25-26 Thin-layer Chromatography Results .. 121

27- Paper Chromatography Results ... 121

28. The Rf Values for "m T c in DEE Medium 133

29- The Rf Values for the ""Vc in Acetone Medium 13^30. Label l ing Y ie l d o f Ol ive Oi l by " " V c O ^ 139

LIST OF FIGURES

Figure Page

1. Anular Number of Patients Investigated by

by Nuclear Medicine in (KKUH) .. ... 3

2. Production of lodine-131 ... ••• 8

3. Decay Scheme of 1 2 3I ... ... 37

4. Decay Scheme of 1 2 5I ... ... 39

5. Decay Scheme of 131| ... ... ^0

6 - 1 6 The Ultra Violet Spectrum Studies for Labelling

Olive Oil ... ... ... 47-50

17- Labelling of Olive Oil with IC1 ... ... 54

18. Labelling of Oleic Acid with IcL . ... 55

19. Labelling of Oleic Acid with Commerical 1C1 — 56

20. Wavelength of Maximum Absorption of IC1 ... 58

21. Labelling of Olive Oil with CAT ... ... 60

22. Labelling of Oleic Acid With CAT ... ... 6l

23*33 IR-Spectrum Results ... ... ... 71-7634. Theoritical Growth and Decay of "Vc in Pure

Parent 9 9Mo ... ... ••• 89

35. The Decay Scheme of " m T c ... ... 91

36. The Decay Scheme of " m M o ... ... 91

37. Linearity Curve ... — ... 107

38. The Spectrum of 33mTc ... ... ... 108

IV

Page

39. The Half-life Curve of " m T c ... ... 104

40-45 Composite Decay Curves of Old Molybdenum-

Technetium Generators ... ... 114-119

46-55. Paper Chromatography Analysis ... ... 123-132

56. Labelling Yield of Olive Oil in DEE ... 141

57. Labelling Yield of Olive Oil in Acetone ... 142

THE AIM OF THIS WORK

LOive oil is composed of many fatty acids, some are saturated and

others are unsaturated. Oleic acid and linolic acid are the most

important two unsaturated fatty acids. Stearic Acid and Palmitic acid

are the most important two saturated fatty acids.

The composing fatty acids, and hence the olive oil, is an

important source of energy for many cells in the body Labelling of

ioc 99mthis oil with radioactive isotopes as IZ-M and Tc helps to study the

metabolism of fats in the body. The labelled oil can be used, as well,

for diagnostic purposes in nuclear medicine and many other medical and

biological purposes.

The ease of giving olive oil in the normal diet, and that it is

free of toxic effect shows the importance of its labelling to be used in

diagnostic and study purposes.

S U M M A R Y

This thesis is composed of two par t s :

Pa «*t 1 : In this part studies related to labelling of olive oil with

125-iodine were carried out.

1251. I was chosen because of its long half-life to represent the

123most widely used I the short-lived one.

2. As the olive oil used in this work contains more than 50% as oliec

acid the latter was investigated as a monitor to the labelling

techniques used.

Among the different methods reported in the literature for labelling

with iodine i the two methods used and applied in this investigated work

were the iodine monochloride method (IC1) and the chloramine-T method.

On labelling using the IC1 method to investigate the labelling,

inactive work was carried first, followed by radioactive work. Using

the IC1 method a yield of >1Q% was found in case of diethyl ether (DEE)

as solvent and at 5 minutes reaction period, for olive oil while it is >8(&

in case of oleic acid under the same conditions. In case of benzene as

solvent the labelling yield reaches a maximum labelling of 37% and >43%

in case of olive oil and oleic acid after 60 minutes reaction period,

vi

after which labelling decrease with time, which may reflect the more

stable the complex of ICl-CgHg than the oil-iodine.

When using CAT a maximum labelling yield of 28% in case of olive

oil in the n-heptane solvent against 50$ labelling yield of oleic acid

under the same conditions of solvent, temperature and reaction time.

When using acetone as solvent it was found that the labelling yield

decreases with reaction time.

Thin layer chromatography technique was applied to determine the

labelling yield.

As a result of IR studies the labelling took place at the double

bond.

Part 2 : In this part , labelling of olive oil with the radioactive

9 9 mTc was studied as well as the radio analytical study for 99Mo- 9 9 m Tc

generator.

It was tried, then, to labell olive oil with the milked 9 9 m Tc. The

results gave a very low labelling percentage yield (only 1.8% ) in

acetone medium. Labelling was tried again using a reducing agent,

SnCl0.2H0O. Labelling yield percentage was compared to the quantityLi it

of the reducing agent in two different media (the acetone and the

VI I I

DEE). A fairly higher labelling yield percentage was achieved in case

of adding 20 mg of the reducing agent in acetone medium. Labelling

yield for olive oil was more than 60% . When the DEE medium was used

under the same conditions, at room temperature, the yield was more

than 50% . It was noticed that the lesser the reducing agent was, the

lower was the yield percentage.

Thin Layer Chromatography Technique (TLC) and Paper

Chromatography Technique were used as quality control systems.

CHAPTER 1 : GENERAL INTRODUCTION

1.1. General

1.2. Artificial Radioisotopes.

1.3. Methods of Labelling of Organic Compounds Vfith RadioactiveIodine Isotopes.

1.4. Olive Oil.

1.5. Historical Cascade of Radioactive Iodine Fatty Adds Labelling.

1.6. Iodine Isotopes and Labelled Compounds.

CHAPTER 1 : INTRODUCTION

1.1 General :

During the past few decades, the progress in nuclear sciences

resulted in the extensive production of radioisotopes, and the wide

range of their applications in industry, agriculture, biology, medicine,

research and many different fields of science and technology. It was

probably in the field of medicine and biochemistry that some of the

earliest applications of radioisotopes have been made, as these were

pronounced to be a new powerful tool in an area of vital importance as

the understanding of metabolic reacions, the mechanisms of the action of

drugs, the location of cancerous growths and obstruction of blood flow.

In fact the scope of the subject would appear to be almost unlimited

particularly in. the presence of specially trained experts and

sophisticated instrucments. Thus in addition to the use of radioactive

tracers in microcurie quantities for monitoring certain processes in the

body, larger doses have been successfully used for therapeutic

purposes for destroying cancerous tissues. For more information

publications can be consulted(l).

The use of radioactive drugs in the Kingdom of Saudi Arabia is

rapidly increasing and especially radiopharmaceuticals labelled with

short-half-life isotopes. These ara frequently produced at hospitals

e.g., King Faisal Specialist Hospital (KFSH) in Riyadh. In King Khalid

University Hospital (KKUH) the amount of radioisotopes applied in the

department of Nuclear Medicine is doubling every year* as shown by

figure (1).

Figure (1) : Anular number of patients investigatedby nuclear medicine in { KKUH).

50Q0

A 000

<Q_

3000

2000

1000

..?•-'"

11t07

Among the most useful labelled compounds are those labelled with

radioiodine isotopes. There are more than 50 compounds labelled by

radioactive iodine-123 (t1/2=i3^3h);odine-125(t1/2=60d), iodine-131(t1/2 =

8d) or iodine-132(t1/2=2.3h) table (1).

TABLE (1) : NUCLEAR DATA FOR IODINE RADIONUCLIDES

USED IN NUCLEAR MEDICINE

Isotope

132,

131I

125.

2.3 hr

8.05 d

60 d

13-3 hr

Half-thickness ofmain y rays in lead

6.5 mm

2.k mm

0.016 mm

0.37 mm

Mode of decay, Energy

B"

B( S") MeV0.2500.3350.6080.815

BE.C(1OO%)

6E.C(1OO^)

668 kev773 kev

Y-rays MeV0.080O.36A0.6370.723

X-rays MeV0.00*»0.0280.035

y-rays MeV0.0280.159

Preparatior

^eactor-ri ssion

Reactor

Fissionproductscyclotron

Cyclotron

1.2 Artificial Radioisotopes

Radioisotopes may be either naturally occuring or artificially

produced.

There are many radionuclides which are clinically useful in

diagnosis or therapy. The energy, the half-life and the type of

emitted radiations as well as the high specific activity are the most

important factors that have to be taken into consideration when

choosing an isotope for a special application. The shorter the half-life

of the radioisotope the more useful it is, since one can repeat the

experiment more than one time during a reasonable period (2). Also the

lower Ihe energy of the gamma emitted from the radioisotope the more

safer is its application. At the same time isotopes emitting only gamma

(Y ) and not beta ( Q ) particles (or low energy beta) are preferred in

medical application in order to decrease the dose affecting the

applicant.

Suitable radionuclides for different medical applications have

gamma energies between 20 to 600 KeV and have physical properties

such that a useable photon flux is available for the examination without

excessive patient irradiation (2).

PRODUCTION OF RADIOISOTOPES

Radioactive nuclides may be prepard by nuclear reactors and by

a wide variety of particle accelerators. However, only reactors or

cyclotrons of at least moderate particle flux are able to produce sources

of sufficiently high specific radioactivities to be of practical interest.

These two methods of production supplement each other in that in

general they do not produce the same isotopes of an element.

1.2 .A-a) Reactor Produced Isotopes ( 3 , 4 , 5 ) :

Experimental nuclear reactors are the main source for more than

90 % of the applied radioisotopes. When a target element is bombarded

with thermal neutrons in a reactor, one or more of the following

processes may occur.

a) The (n, gamma) process, in which a neutron is captured by the

nucleus of a target atom, and almost simultaneously one or more gamma

photons are emitted. The target atom is changed to an atom with one

more neutron in the nucleus, that is , to a heavier isotope of the same

element. The process may be represented symbolically as follows:-

2 X, (n,Y) +2X

b) The (n, P) reaction : A target nucleus absorbs a neutron and

expels a proton immediately. The product atom is therefore an atom of

an element with an atomic number lesser by one than the target

element, and the same mass number, giving a carrier free isotope, a

symbolic example is:

c) The (n, gamma) process followed by radioactive decay to the

desired product. The produced isotope is of high specific activity and

is carrier free. An example is the production of Iodine-131 by

irradiation of tellurium dioxide (TeO») or any tellurium target.

Figure (2) shows the production of Iodine-131 in a neutron flux of13 2

5x10 n/cm /sec, target tellurium metal.

130Te (n , Y )

d) The (n, a ) process : A neutron is absorbed and one or more

alpha particles emitted.

ZX (n,a) Z .2Y

It might be mentioned here that a number of stable nuclides can

be produced by neutron irradiation that could not otherwise be obtained

in pure form. For example:

1 9 7 A u ( n , Y ) 198Au B-d e C a^ 1 9 8Hg

e) Fission : As a result of uranium fission a tremendous amount of

Specific Activity (Curies per gram of Tellurium)

IO

\n 3 -tin> - i

x cort a.— -\ co o o

— 3 rt

- 3O

VIno

rtQl-1

••anrt

n— oic

oQ.

3ni

9 ow 9

01

?t i

on

2" 8

s\

\

00

activity can be produced. All fission products are Beta emitters. Some

of these radioactive fission products can be obtained in substantial

quantities by chemical separation from the residual uranium and other

elements present in the burnt-out reactor fuel rods. For instance:

U(n, Fission)

f) The secondary nuclear reactions : In these reactions the target

material is admixed with another material suffering any one of the last

given nuclear reactions, then using the emitted, p,ct to initiate a

nuclear reaction in the target material thus using a reactor as source

of charged particle instead of a source of neutrons. For example

mixing the target material with Li, and according to the nuclear

equation Li( n' a) T, one can make use of the charged a particle or

the tritium to intiate another nuclear reaction, of course this procedure

gives low activity, but is of value in absence of accelerator facilities.

1.2.A-b> Some Theoritical Aspects of Radioisotope Fvoductioii(3,4,5):

The theory of reactor irradiations is, in general, extremely complex.

Some of the elementary aspects will be dealt with here. The probability

that a certain incident neutron will be captured by a certain atom of

the target material depends on the energy of the neutron and on the

characteristics of the target nucleus. If we know the energy of the

10

neutron (usually thermal energy) we can express the probability of

capture in terms of an imaginary small circular area surrounding the

target nucleus and perpendicular to the path of the neutron such that

if, and only if. the neutron passes through the area, capture occurs.

This area is called the capture cross section of the target nucleus.

The capture cross section is different for different target nuclei and

for different neutron energies. In almost all cases, the slower the

neutron is travelling (i.e. the lower its energy), the greater is the

probability of capture. The thermal neutrons, which are slowed down

to the lowest possible energy for a neutron are therefore ideal for the

purpose. The cross section area is usually expressed in barns

-24 2(1 barn = 10 cm ). The thermal neutron cross sections of a number

of target materials are tabulated and published in many reports edited

by the International Atomic Energy Agency, Vienna (IAEA).

From these considerations, we can readily show that after a

target material is exposed to thermal neutron irradiation for a time t,

seconds,its specific activity at any time during irradiation is equal to:

1 l /

Activity = 0.602 ijoa A"1 (l-(l/2) l * ) Bq . g

t1.62 x 10"1 ] 0 a a A ' 1 ( 1 - ( i ) / t : i ) Ci .g " 1

11

The activity at any time after end of irradiation is

Activity = 1.62 x 10"11 0$ a A~1(1-(1/2J ^i ) (1/2)

where $ = neutron flux in n/cm2/sec.

a = thermal neutron cross section of the target material in cm2

A = mass number of the target element

a = the percent natural abundance,

t = time of irradiat ion.

T = cool ing time,

t , = hal f-1i fe time of the isotope of interest.

Knowing the characteristics of the target material and the

thermal neutron flux, we can use the last equation to calculate the

specific activity of the target after any irradiation time. The time

needed to produce a given specific acitvity depends on the thermal

neutron flux, the cross section and the rate of decay of the product.

In practice irradiation times vary from a few hours to 2 or 3 years.

The specific activity calculated by the last equation must be corrected

to allow for several sources of error. The actual activity produced is

usually less than the calculated value. The ratio of actual to calculated

activity is called the irradiation efficiency. Practical irradiation

12

effeciencies may be as low as 20% or as high as 80% depending on the

self-sheilding in the target material and /or on the burn up factors.

Irradiation efficiency can not in general be predicted by theoritical

means. In practice predictions are based on empirical factors derived

from the results of past irradiations. These include certain factors

which are :

i) Day-to-day variation in the neutron flux due to shielding by other

target materials in adjacent reactor position and to unscheduled

variations in the reactor power level.

ii) Impurities in the target. '

1.2.A-c) Practical Aspects of Reactor Irradiations (3,4,5):

In theory, almost any nuclide can be converted to another

nuclide by neutron irradiation. Whether or not this is feasible or

worthwhile depends on a number of factors.

Some target materials can not be irradiated safely at normal

reactor temperatures of several hundred degrees. Substances that are

explosive, pyrophoric or extremely volatile at such temperatures are not

in general acceptable as targets. If the target isotope has a very low

activation cross section an unpractically long irradiation may be required

13

to produce appreciable activity. If the radioactive product has a very

short half-life it may decay as fast as it can be produced, or before it can

be shipped to the user. The amount of a given target material that can

be put into any one reactor position is limited by a number of factors.

For example the design of most reactors leaves only a very limited amount

of space for radioisotope production and hence volume is an important

restriction.

1.2-B Accelerator Produced Radioisotopes (3,4,5):

Whereas a reactor can only give a flux of neutrons and gamma rays,

accelerating machines can use many other types of bombarding particles.

These are charged, generally, positively, although electrons are also

accelerated, and include protons, deuterons and heavy ions. There are

several types of accelerating machines, sometimes given the generic term

"cyclotron" and differently named according to the particle accelerated and

the mode of doing this. In general, a beam of charged particles is

injected at one point, and by being subjected to electric and magnetic

forces is accelerated either in a straight line, or, more commonly in a

spiral path increasing in energy as it does so. The high energy particle

strikes a target and may impart sufficient energy to cause a nuclear

reaction. Bombarding with protons or deuterons can produce new nuclides

with an excess of positive oharge, for instance the bombardment of

boron-10( B) with deuterons produces carbon-11 ( C), which is

radioactive and emits B particles. At high energies, enough energy may

be imparted to cause a break-up of the nucleus termed "Spallation" as in

case of 37Cl(P,6P4n)28Mg.

The main points about accelerator produced isotopes are :

a) The resulting nuclides decay by g or by electrone capture (E.C.)

modes.

b) There is a change of element, so the products are carrier free and

need chemical extraction from the target.

c) The target becomes considerably heated, and this either limits the

choice of material or necessitates special cooling, or both.

d) The beam is small and so the number of targets that can be irradiated

at one time is limited.

e) The yield is a function of time and beam current (flux and time in

reactor irradiation) and of course it depends upon the cross-section for

the reaction, which raay in turn depend upon the particle energy.

f) Becuase the output of radionuclides is small, the cost of production

tends to be high. However some nuclides produced by this route have

15

properties which are more suitable for some purposes than reactor

produced radioisotopes of the same element.

A radionuclide which has achieved importance in recent years for190

body function studies, is iodine-123 ( I ) with a half life of 13.2 hours

and emission of gamma rays of energy 159 KeV with no particle emission

(table 1). The half-life is of reasonable length, and the dose to the body

is less than is given by comparable activities of any other iodine

radioisotopes. It is produced at AERE Harwell using 58 MeV protons in

the variable energy cyclotron,

%

72% EC j, 1 2 3I n+

Auger effect

28% 6 + 123T-

1 2 5X e Auger effect

the target material is di-iodomethane.

123A very good review of I production methods is given by

Stocklin(6).

1.2-C Radioisotope Generator Systems (3,4):

Several short lived radioisotopes which are useful in clinical

radioisotopes work are the daughters of longer-lived parents. In fact it is

preferable to conduct trace experiments with short-lived nuclides as Lhis

16

eleminates the problem of disposal of residual radioactive waste after

completion of the experiment. It is convenient to have a long-lived

mother in storage from which a short-lived daughter can be removed as

required for use in tracer work. A few examples of uses of such

mother-daughter can be removed as required for use in tracer work. A

few examples of uses of such mother-daughter pairs are included in

Table 2. Such systems are called radioisotope generators.

132Most commonly used radioisotope generator is Te from which•too 132

I may be milked. In this case Te is adsorbed as radium tellurite132on an alumina column, and the I removed by passage of 0.01M132ammonia through the column. The I is used both diagnostically and

therapeutically for thyroid cancer, (k)

Another commonly used radioisotope generator-milking system99 99Mo- Tc is used for diagnostic purposes for liver, spleen, and other

99scanning. The Mo parent is absorbed on a column of alumina and the

daughter ' mTc removed by passage of saline solution at intervals

governed by the equilibrium. The parent, when it is fixed in a

semi-permanent sample as on an adsorbent column, is often known as a

"cow" and the removal of the daughter activity from the radioisotope

generator (the "cow") is termed milking (see part 4 of this thesis).

TABLE (2) : SOME COMMON RADIOACTIVE MILKING PAIRS. THE DECAY PROPERTIES INCLUDE DECAYENERGY (MeV),MODE OF DECAY AND HALF-LIFE,

Mothernuclide

DecayProperties

Daughternuclidc

DecayPronerties

Application

44Ti

68Ge

90Sr

" ]

113

132

137

140

144

210

226

238.

Sn

Te

Cs

Ba

Ce

Pb

Ra

EC,Y:47.3 y 44Sc

68EC:275 d

O.5S0;28.1 y

3.YJ284 d

P.YJ21 y

a; 1600 y

a; 4.5x109 y

Ga

1 3 7 m Ba

140La

144Pr

210Bi

222 Rn

l.SB ;1.17:4.0 h

1.886+,1.O8Y5

1.14 h

2.27B;64 h

0.14Y;6.0 h

0.40YJ1.66 h

3,Y=2.3 h

0.28Y.2.55 min

3.00g;17.3 min

1.163;5.01 d

a;3.82 d

B.YJ 24.1 d

Teaching

Medical

fa")Heat source (large amounts). '

calibration source

Medical

Medical

Medical

Gamma radiography, radiation . ..sterilization (large amounts) '

Lanthanum tracer

Calibration source

Calibration source

Medical

Thorium tracer

(a) Mainly use of mother substance.

Reference CO

18

1_3 ifethods of Labelling of Organic Compounds With Radio-active Iodine

isotopes (7):

A radioactivity labelled (or "tagged") compound is one in which one

of the atoms is radioactive. Preparation of labelled compounds may

involve lengthy chemical synthesis starting with the radioactive nuclides

in elementary form or in a simple compound. Labelling is said to. be

specific when only one position, in the compound, contains radioactive

nuclides. However labelling is said to be general when several

positions are labelled. Labelling is said to be taking place through

biosynthesis when the complicated organic compound is left to grow in a

substrate containing the radioactive nuclide.

The use of radioisotopes for labelling of organic compounds have

been adapted to a large extent becuase the isotopes are available and

these labelled compounds play an important role in nuclear medicine (8).

High specific activity is desirable for the radiopharmaceuticals so that

nonphysiologic amounts can be administered. For radio-immuno-assay

high specific activity is important for sensitive assays.

Radioiodination of protein has generally been carried out by one of

three methods: the iodine-mono-chloride (IC1) method (9, 10, 11); the

Chloramine-T method (12, 13, 9); and the electrolytic method (14, 15).

Procedures for iodination of fibrinogen by IC1, Chloramine-T and

electrolytic methods have been published (16). Reaction yields for

radioiodinated fibrinogen were measured by separating labelled

fibrinogen from free iodide ion using a sephadex G-10-12 gel

chromatography column (16). Krohn and Welch(17) have reported the

carrier-free iodination of fibrinogen with percentage yield ranging from

60-85% within 30 min.

Other procedures were recorded in the literature for labelling of

proteins depend on freeing the I in direct contact with the protein by

oxidation of KI solution. The oxidizing agent such as KIO_ (18, 19),

nitrous acid (20), hydrogen peroxide (21), ammonium-persulphate (22),

chloramine-T (23) have been reported in the literature. All these

oxidizing agents are able to induce denaturation phenomena becuase

they are in direct contact with the protein solution. To avoid the

denaturation of the product, labelling methods in heterogeneous phase

have been adapted (20, 24). Therefore a new method was described125for labelling proteins to high specific activities with I (25). This

new method involves reacting the protein under mild conditions with the

N-hydroxy-succinamide ester of 3-(4-hydroxy-phenyl) propionic acid125that has previously been labelled with I and separated from the

products of the iodination reaction by solvent extraction (26).

Enzymatic oxidation has been developed for the iodination of

proteins (27) and immunoglobulins (28). The enzymitic oxidation

was also utilized in labelling of gonadotropin (29),

20

aromatic steroids and other hormones and proteins (30). This method

requires the reaction of Ijactoperioxidase, carrier-free radioiodine and

the compound to be labelled together with nonmolar quantities of HnC>2

It yields high specific activity products and the biological activity for

radioimmunoassay is preserved (28).

Another important class of methods for introducing radioactive

iodine and bromine into a molecule is the halogen exchange (31). In1O1

1966, Tubis et. al (32) first described the preparation of I labelled131Sod-o-iodohippurate by isotopic exchange between Na- I and inactive

o-iodohippurate. Radioiodine labelling of o-iodohippurate by isotopic

exchange was further studied by Scheer et. al. (33) and in more

details by Hallaba et. al. (34). Various procedures for the separation

and purification of labelled o-iodohippuric acid after exchange labelling

were described (34-36). A new technique for iodine labelling of

aromatic iodine compounds has been described and applied to the131preparation of I-labelled m-iodohippuric acid (37). m-iodohippuric

acid is of great stability and has advantages for nuclear medical

application when compared with o--iodohippuric acid. The method is

very efficient, and in this particular case the exchange is completed

within about 30 minutes at a temperature of 161° C.

A new approach has been reported under the name "melt method"

(37). Isotopic exchange by the melt method in general is very efficient

21

and fast (37-39), if the reaction proceed without decomposition of the

compound to be labelled. This method was used to prepare radioiodine123

labelled o- I HA with radiochemical yield of almost 100% (40).

On the other hand, there are some cases in which the compound to

be labelled decomposes during melting (31). To avoid this phenomena

low melting derivatives of the compound have been used (31).

123Lambrecht et. al (41) used the decay of Xe in the exchange labelling

123 123

in the melt to prepare 1-4-iodophenylalanine, I-5-and-6-

iodotryptophan. Further utilisation for this approach have been

developed by Elias and Lotterhos (7), who used "unreactive" solvents

(acetamide) which has low melting point and a good solubility for many

organic compounds as well as for metal halides. It was found that, the

radiochemical yield observed after two hours at 180° C is 80% for

exchange bromobenzoic acid to m-iodcbenzoic acid (41, 7).

For many medical application products, iodine-131 or iodine-125

radiopharmaceuticals which are presently being used for "in vivo"

procedures can be replaced by iodine-123 due to its convenient

characteristics. Table (3) summarizes the most important used

practical labelling procedures.

22

TABLE 3 : METHODS OF LABELLING

T h e r e a r e e s s e n t i a l l y f i v e m a j o r t e c h n i q u e s e m p l o y e d i n t h e

p r e p a r a t i o n o f l a b e l l e d c o m p o u n d s f o r c l i n i c a l u s e : {k2)

METHODS EXPLANATION EXAMPLES

Isotope ExchangeReactions

In these reactions, one or more atoms ina molecule are replaced by isotopes ofthe same element having d i f f e ren t massnumbers. Since the radiolabel led andparent molecules are ident ica l exceptfor the isotope e f f e c t , they are expectedto have the same b io log ica l and chemicalpropert ies.

3 2 S-

and 3H-labelledcompounds

Introduction ofa foreign label

In th is type of l a b e l l i n g , a radionuclideis incorporated into a molecule that has aknown biological r o l e , p r imar i ly by theformation of covalent or coordinate-covalent bonds. The tagging radionuclideis foreign to the molecule and does notlabel i t by the exchange of one of i t sisotopes.

" m Tc- labe l l edalbumin.5 l Cr- labe l ledred bloodc e l l s .1 3 1 | - l abe l l edproteins.1 2 5 l - l abe l l edfa t t y acids

Biosynthesis orchemical synthesis

In biosynthesis, a l i v i n g organism isgrown in a cul ture medium containingthe radioactive t racer ; the tracer isincorporated into metabolites producedby the metabolic processes of theorganism, and the metabolites are thenchemically separated.

5760C0 orlabelledvitamin B

CO-

12.1 C-labelledCarbohydrates,proteins, andfats.

Continued....

Table (3) continued

23

METHODS EXPLANATION EXAMPLES

Recoil labelling This method is of limited interestbecause it is not used on a largescale for labelling. In a nuclearreaction, when particles are emittedfrom a nucleus recoil, atoms areproduced that can form a bond withother molecules present in the targetmaterial. The 1ight energy of therecoil atoms results in poor yieldand hence allow specific activity ofthe labelled product.

H-labelledcompounds.lodinatedcompounds.

Exitat ionlabel 1 ing

(from 1 2 3Xedecay)

This method of labelling entails the 1231 —labe1 ledutilization of radioactive and highly compoundsreactive daughter ions produced in anuclear decay process. During gdecayor electron capture, energetic chargedions are produced that are capable oflabelling various compounds of interest.77 77

Kr decays to Br and, if the compoundto be labelled is exposed to 7 7Kr, thenenergetic 7 7Br ions labelled the compoundto form the brominated compound.

24

1-4 Olive Oa

Olive oil is one of the natural oils, it is obtained from ripe olives,

the fruit of the cultivated olive trees. The olive oil is a pale yellow oil

with a pleasing delicate flavor. It has a density of 0.909-0.915 at 25 C

Iodine value for olive oil is 79-90 (43).

Olive oil is a mixture of glycerides. It is composed of many fatty

acids, (Table 4). Some are saturated while others are unsaturated.

TABLE : OLIVE O I L COMPONENTS

Sa

tura

ted

Un

sa

tura

ted

Fatty Acid

Palmi tic

Stearic

Otheis

Oleic

Linoleic

Others

Structure

C15H31COOH

C,7H35COOH

CH (CH2) CH=CH(CH2) COOH

CH (CH2) CH=CHCH2CH=CH(CH2) COOH

Percentage

a 10.0%

b 12.95%

a 3.3%

b 2.83%

a 0.6%

b 2.27%

,a 77.5%

b 58.12%

a 8.6%

b 13-69%

a

b 6.M»%

25

The main constituents of olive oil is oleic acid (9-octadecenoic acid)

Co H,. 09 ; the chemical structure is as below :18 oi L

C H 3 ( C H 2 ) 6 C H 2 - ^ —-V'Y-

Pure oleic acid is colorless, of density about C.895 at 25° C, and

the iodine value is 89.9 (43).

The distribution of olive oil in rats tissues was done by Cappelli

(44), to study the functional and biochemical effects of olive oil. The

study shows the relative weight of olive oil expressed as percentage

body weights of rats fed with olive oil (see table 5).

TABLE (5) : RELATIVE WEIGHT OF OLIVE OIL EXPRESSED

AS PERCENTAGE BODY WEIGHTS OF RATS FED WITH OLIVE

Heart

0.23

Liver

2.35

Kidney

0.5't

Spleen

0.22

Testes

0.80

Another study was done to determine the fatty acids of myocardium

of rats fed with olive oil. Table (6) shows the results given by

Beare-Rogers (45)

TABLE (6) : PRINCIPAL FATTY ACIDS OF

MYOCARDIUM OF RATS FED

WITH OLIVE OIL.

26

Fatty Acid

Carbon atom No. / double bonds

16:0

18:0

18:1

18:2

20:1

20:4

22:5

22:6

Percentage

12.2

22.1

18.3

14.4

0.2

17.4

2.1

9-5

Total Fatty Ac ids/Myocardium (mg/g) used= 15-4

27

Many other studies about the distribution of halogenized olive oil in

experimental animals are mentioned in the literature. (46,47, 48,).

These studies showed the presence of olive oil components in the liver,

kidney, heart, spleen, and testes. This wide range of distribution

shows the importance of labelling of olive oil with radio-active isotopes

for diagnostic purposes.

1.5 Historical Cascade of Radioactive Iodine Fatty Acids Labelling :

Fatty acids are one of the main sources of energy production in

mammals, and their physiological and biochemical fate has therefore been

extensively studied. Recently new attention has been focused on these

compounds because, if labelled with suitable emitting radionuelides, they

may be used to monitor part of the energy producing metabolism in vivo

(49).

Radioiodinated triolein and fatty acids have been widely used in the

assessment of intestinal malabsorption and maldigestion.

The method of study is essentially a tracer test in which a known

dose of radioiodinated triolein and oleic acid are orally administered and

the percentage of the ingested fat and fatty acid appearing in the blood

or excerted in the fecal samples is measured. This provides a

28

diagnostic aid in assessing fat digestion and absorption by the

alimentary tract (50).

In 1949 Stanley (51) studied the absorption and desorption of orally131 131

administered I-labelled olive oil. He had mixed I with carrier

and acid, then the liberated iodine was extracted with chloroform. Into

the chloroform solution a stream of chlorine was then passed until the

purple color of iodine just disappeared. The iodine chloride obtained

was added to a chloroform solution of 20 gins, of olive oil. The labelled

olive oil was soaked into bread and eaten.

131Later on, Tuna (52) et al. have used I to radioiodinate triolein,

olive oil, sesame oil, and peanut oil. The various samples were

analyzed chromatographically for radiochemical purity. It was found

that only 30 to 60 percent of the radioactivity was in triglycerides.

Remaining radioactivity was distributed among free fatty acids, their

methyl esters, partially digested fats, acetoglycerides, and other

substances, then the absorption in human body was studied.

In 1970 Davila and co-workers (53) described a new method of131preparing I-labelled oleic acid and triolein which may be used for

studies on the absorption and the metabolism of fats. In this method

the labelling of the compounds and the subsequent separation and

purification of the labelled products were done in one vessel in a

continuous manner.

29

131The absorption of I-labelled oleic acid was studied by Turk (54).

The labelling have been done in a second gelatin capsule containing 20131uCiof I-labelled oleic acid whi<

the radio-zinc containing capsule.

131uCiof I-labelled oleic acid which was administered concurrently with

131Tennant et al (55) demonstrated the absorption of I-oleic acid131and I-triolein by germ-free and conventionalized rats and it has been

demonstrated that there are several differences in lipid metabolism

between germ-free and conventional rats. To evaluate the role which

intestinal absorption might play in determining these differences, they

compared the absorption of I-oleic acid and I-triolein in germ-free

and conventionalized rats. Gastric emptying of both compounds

appeared to be delayed in germ-free rats and correspondingly less

radioactivity reached the cecum during the 6 hours period following

intragastric administration. When corrections were made for differences

in gastric emptying, germ-free and conventionalized rats absorbed oleic

acid and triolein at similar rates. Under the conditions of their

studies, intestinal micro-organisms did not appear to influence the rate

of either lipolysis or fatty acid absorption directly, but significantly

influenced the rate at which fat was transported along the gastro-

intestinal tract.

Eugenio (56) et al. used a technique for labelling oleic acid using

reactor-irradiated coconut oil resin (RICOR). The most effective

30

technique for labelling oleic acid now in vogue employs iodine131monochloride tagged with I to introduce radioactive iodine into the

oleic acid molecule. In this work they presented a technique using

RICOR and oleic acid molecule was labelled with radioactive iodine. It

appears that RICOR can be used as an effective medium for labelling131oleic acid with I. This new labelling technique is fast, easy and

convenient to use provided that the iodine concentration in the final

product is not too critical.

Robinson and Lee (57) used radioiodinated fatty acids as agents for

use in heart imaging. Previous studies in experimental animals and131humans using I-oleic acid of low specific activity were marginally

successful. Higher specific activity compounds offer potential

improvement for use as imaging agents for normal myocardium.

The labelling of oleic acid with 1 4 C , 1 3 1 I and 131I-labelled linoleic

acid have been described by Beierwaltes et al (58). The distribution of

131I-labelled oleic acid or linoleic acid was also studied in dogs.

Radioactivity concentration in the myocardium was the highest at all131times, the myocardium uptake of I-oleic acid was significantly higher

than the radioactivity in the blood or other tissues at 30 minutes after

injection.

31

131Robinson (59) has synthesized I-16-iodo-9-hexadecenoic acid by

123reacting the brominated precursor with I-iodide under reflux in

anhydrous acetone or methyl ethyl ketone (MEK). I-iodide was

extracted into the reaction medium from aqueous (4N) NaOH single

extraction transfer into acetone which was more efficient than into MEK,

but labelling yields were higher using MEK.

131 125Norman et al (60) used I, I and some radionuelides to label

hexanoic acid, oleic acid and stearic acid. They used the labelled

compounds for myocardial imaging.

123 11Machulla and Stoklin (61) prepared I and C labelled long-chain

fatty acids for kinetic studies of heart muscle meatabolism.

14Machulla et al (62) labelled various long-chain fatty acids with C,

34 77 123Cl, Br, and I and evaluated their protential application in

measuring myocardial metabolism in vivo.

Otto et. al. (63, 64) studied terminally iodinated long-chain fatty

acids and it has been used experimentally and clinically as myocardial

imaging agents. Six u-iodo fatty acids (I(CH2)n COgH where n=10, 12,

15, 18, 21, 26) have been synthesized and tested in rats. Myocardial

extraction values and heart-to-blood ratios are affected by chain length

and they found that the radioiodinated fatty acids have short myocardial

32

tn ,„ and high blood activity levels when these used as myocardial

imaging agents. Both of these problems may be related to rapid

8-oxidation of the fatty acids by the myocardium and liver. They

suggested several approaches to decrease the rate of g-oxidation. One

approach is to modify the carbon skeleton to promote storage as

triglycerides.

A description of a rapid method for labelling long-chain fatty acids131 123

which gave high rpecific activity with radioiodine ( I or I) wasgiven by El-Shaboury (65).

In 1982 Riche (66) labelled fatty acids with iodine 123 or 131 in

w-position. This worker has developed a simple and rapid labelling

method which requires no product purification and should therefore be

routinely useful in nuclear medicine laboratories. The synthesis of long

chain fatty acids iodinated in u-position is performed by tosylation of

the u-hydroxy acids followed by an exchange reaction.

The problem of deiodination of long chain fatty acids results in

relatively rapid loss of radioactivity from the myocardium with

accumulation of radioiodide in the thyroid and blood. In order to

overcome the problem of radioiodide loss, iodine has been chemically

stabilized by attachment to the para position of the phenyl ring or by

the introduction of the tellurium as a heteroatom in the fatty acid to

33

inhibit 8-oxidation and "trap" the fatty acid in the myocardium.

Knapp et al (135, 136) prepared two new tellurium fatty acids in which

iodine-125 has been chemically stabilized by attachment as a trans-vinyl

iodide (I-CH = CH-R-Te-It -COOH) and evaluated them in rats. The

absolute heart uptake of this agent was moderate, but the hearfblood

ratios were low. The effect of tellurium position was unexpected and

the heart/blood ratios were dependent upon the position, of the

tellurium.

The preparation of terminal p-iodophenyl-substituted- a and

g-methyl-branched long chain fatty acids have been described by

Goodman et al. (137). The radioiodinated agents are of interest as a

result of the expected pronounced uptake and prolonged myocardial

retention that may result from the inhibition of fatty acid metabolism.

A comparison of the heart uptake of the radio-iodinated

methyl-branched fatty acids and their unbranched analogues has

demonstrated a greater myocardial retention of the methyl-branched

fatty acids than the unbranched analogues. The tissue distribution

studies in rats have been done.

1.6 Iodine Isotopes and Labelled Compounds :

There are 25 radioisotopes of iodine, ranging from atomic mass 117

to 137. The potential of each of these is discussed by Mayers (94).123For various reasons only four have become important. These are I,

131j a n ( j 1 j_ Nuclear properties as well as method of production

of these radioisotopes are shown in tables (1,8,9,10) and figures

(3,4,5).

ioi no

I and/or I are produced by neutron irradiation of tellirium235targets or separated from fission products of U. Iodine-125 is

124produced by neutron irradiation of Xe or by accelerator.

Although Iodine-131 has been used more often in clinical studies123 125 132

than I, I or I, becuase of its availability, low costs andrelatively long half-life yet iodine-123 is competing because of its short

131half life, low y energy and non-beta particles. With I a 364 KeV

photon is emitted 80% of the time, but higher energy photons of 637 and

722 KeV are emitted about 12% of the time with resultant septal

penetration in collimators designed for lower energy emissions.

Iodine-125 became commercially available relatively late in 1960s.

1-125 has been shown to produce thyroid scans, at least, as good as

those of 1-131 in resolution and sensitivity. This isotope however

became popular after invention of (RIA) radio-immuno assay (69, 93).

There are many compounds labelled by Iodine-125; some of these

compounds are shown in Table 7.

35

TABLE 7 : EXAMPLES OF COMPOUNDS LABELLED WITH

IODINE-125 AND THEIR APPLICATION(S)

Compounds labelled

withApp)ication Reference

Meta-D imethoxy-N,N-Oimethyl lodophenylIso-propy1 ami nes

Imaging agent fo r brainblood flow

Mathis, C(72)

co-lodo Fatty Acids

l(CH2)nCOOH

(n=10, 12, 15, 18,21, and 26)

13-lodo-3-methyltridecanoic acidi6-Bromo-9, 10-methylene-hexadecanoic acid

iA-iodo-9~tetradecanoicacid

Myocardial Imaging Agents Otto, C.(6M

15-(P~lodophenyl)-6-Tellur apentadecanoicacid

17-iodo 9-tellurahepta-decanoic acid

For the diagnosis ofheart disease and todelineate regions ofabnormal fatty acidmetabolism within themyoca rd i urn

Knapp, F. (135)

i8-lodo-13-tellura-17-octadecanoic acid

17-1odo-heptadecanoi cacid

17-lodo-9"tellurahepta-decanoic acid

i6-lodo-9~Hexadecanoicacid

15-(P-lodophenyl)Pentadecanoic acid

O-T«»I 1 •"-=>ri-h»ntadecanoic

Determine themyocardial uptake

Knapp, F. (136)

Table 7 (Continued)

36

Compounds labelled

with 1 2 5 IApplication Reference

5-Ben zoxy-1 -Pen ten e

3-(P-tolythiol)-2Methylpropene

i8-nonadecenoic acid

21-docosenoic acid

Diagnostic nuclearmedicine

Kabalka, G. (68)

A-iodobenzyl bromide

l»-trimethylsi ly l benzylbromide

For label l ing otherbiological ly importantmolecules which possessuitable nucleophil icfunctional groups

Wilson, A. (67)

T»-(P-iodophenyl)2(RS)-methyltetradecanoic acid

Myocardial imagingagents

methyl-pentadecanoicacid

19c

[ I ] Iodospiroperidol

Goodman, M. (137)

Fibrinogen

Human Albumin

Plasma AlbuminProteins

To study fibrinogenbehavior in vivo

For metabolic studiesand behavior of theprotein

For metabolic studies

Krohn, K.

Rosa, U.

Katz, J.

(7*0

(15)

(70)

For use in v i t r o assaysto consider theY emitting dopamineantagonist

Laudvatter, S.(73)

Amidarone (Cordarone ) For medical uses Sion, R. (71)

37

Table (8) : Reactions realized by the use of an accelerator

(Production of 123l)

Reaction

™Te(p.n)ml

•«Te(p.8n)'"l

••'Te(>He.2n,'»XeE-?'»I

'»Sb(>He.3n,»M

'!'Sbfo.2n)'"l

«'Te(a.3n,'»XtE-C=»I

Abundanceof argetnuclide

0.87

31.79

34.49

2.46

41.75

57.25

2.'6

Energy ofincidentpaniclei(MeV)

15.5

15

80 [8]

30

30

25

30

d30-35[11]

46 [12]

Productionrate

ixiCi/mAh

-450 b [3]

-1000 C [7]

-90CC [7]

-300 C [7]

200 [9]

40-120 [10]

Side reacDor.1 ir.chalf-kit s!

nuclide fanned

mTe(p.n)»'ltTj = 1.3 h)iiot. abund.: 0.06K

"'Tecp.n)1"!

iioi. abund.: 4.61".-

m Te(p .n) '" l(Tj • 60.2 d)isot. abund.: 6.99^

(Tj = l l . e d )iiot. abund.: IE.TIT.-

'"Tetp.n)'"!

iioi. abuni.: 34.49C>

•"Sbfe.n;"'!

iiot. aounc.: 42.75-T-

"•Sbfo.aro"*!

"'1 . " M a n i ' * l

reactions

FOT all nuclear aata except those with their own reference, tee Ref.fj3 & Ja Only iide reactions producing nuclides with half-livei excee^mc 1 hare taken into con:ideri£cr.^ Refen 10 approx. "50 mg of tellurium enriched in 1IJTe to SPC-.c Tfic weight of targe: >nd its enrichment not given.0 The optimum ranee c! energy for production.

t.«3

B.33

11.11

0.14

. i

38

TABLE (9) : Reactions realised by the use of an accelerator

125(Production of I)

Reaction

»Te<p.n)«l

"•T«(d.n)m l

«»Te(d.2n)'»l

'"Sb(o.ai)">l

iKHOpIcabundance

olihemiclide

<*>

6.9!)

4.6)

6.99

42.15

Energyof incident

panic lei(MeV)

16- IB

to

14

30

Production rate(mCi/mAh)

1.8 [7]

1.0 18]

15.0 (9)

0.42 [10]

Secondary reaciioniand hall-lire of the

nuclide formed

mTe(d.n)"MCTj • 13.8 d)lut. abund.: 6.99

"'SKn^n)111!(TJ = S.>2h)ilol. abund.: 57.25

'"SKa.anl1"!(Tj • 13.3 h)

'"SWn.an)1"!

'»Sb(e..n)lwI(Tj • 12.8 d)

39

Table (9) : Reactions realized in a nuclear reactor

(Production of 1 2 5|)

Reaction

l"Xe(n.))mXe

liotopiabundance

oruenuclide

(*)

0.096

C«MJ-

tection(bam)

110

Activity of elementat 10" n/cm'-i

(Cl/g)

1 week S week u i .

0.22 0.45 Z.B

Secondary reaction!and half-life of theradionuclide loaned

'"Xetno^'xe{Tj » 3 6 . « d)iiot. abund.: 0.09o * 2 bam

(Tj «B.0d)itot. abund.: 1.9:o < 5 bam

l"xe(n.T) I > 1Xen i

( T ) - l l . B d )iiot. abund.: 4.08a < 5 bam

(T, • S.27 d)iiot. abund.: 26.B9o < 5 bam

"*Xe(n.})"*Xem

(Tj = IS. 6 min)iioi. abund.: 10.4o < 5 bam

(TJ « 9.14 h)o - 0.2 barn

(Tj - 3.9 min)isot. abund.: B.S7o - 0.1S bam

For nuclear data m Rd.[95 J

125 TS3*

0.03S4S

Figure (A) : Decay scheme (MeV)

Table (10) : Reactions realized in a nuclear reactor

(Production of 1 3 1|)

Reaction

l"Te(n.))n'Tem

\30 h

IT 18% '"I

24.8 min

.1 Z8'

A un ance

of targetnuelidt

(To)

34.49

34.49

Croii-section(barn)

0.04

0.2

Activity of elementat 10" n/cm1'!

(mCi/g)

24 h 7 d ut.

1.4 7.9 n . S

7.2 40.0 S9.0

Side reactions andhalf-life of

nuelide formed

'»Te(n. 7 )" ! TeCTj • 11 d)lKJl. abund.: 0.D8?fro " 0.3 bam

m T e ( n . T ) 1 " T e m

CTj • 1M U)a * 2.0 bam

mTe(n.r)v l lT em

(Tj • i n d)iut. abund.: 2.46^o " 1. 0 bam

iioi. abund.: 4.61%0 * S.Obarn

( T j - 9.4 h)Uoi. abuni.: 18.111a * 0.9 barn

IMTe<n.i)1"T!m

(Tj a 109 d)o=0.1 barn

mTe(n.,)1MTe(TJ - 6S.:rmn)isot. abund.: 31.1?>c0 • 0.14 barn

(Tj •= 34.1 dlo = 0.011 barr.

For nuclear daia xee I

•s

11

C.JI5

1

i .

O.IH

1•. t

- a. TO

— 0.3M

i x .

Figure (5 ) : Decay scheme (MeV)

CHAPTER 2 : EXPERIMENTAL and RESULTS

2.1 The Iodine Monochloride Method.

2.2 Labelling of Oil with Inactive Iodine Monochloride Method.

2.3 Labelling of Oil with Radioactive Iodine Monochloride Method.

2.4 Labelling of Oil With Chloramine-T Method.

2.5 Quality Control Systems.

CHAPTER 2 : LABELLING OF OIL - EXPERIMENTAL AND RESULTS

In this work two methods were investigated aiming at preparing

labelled olive oil and/or oleic acid with radioactive iodine. The methods

used are the iodine monochloride (IC1) method and the chloramine-T

(CAT) method. The theoretical base of these methods are:

2.1. The iodine monochloride (IC1) method :

If potassiumiodate solution is added to potassium iodide solution in

the presence of hydrochloric acid (HC1), the reaction occurs:

2KIO, + 10KI + 12 HC1 = 12 KC1 + 6I_ + 6HOO (1)

However, if an excess of concentrated HC1 is present, a further

quantity of KICL oxidizes the I_ to IC1 according to equation (2).

3KIO3 + 6I2 + 18HC1 ?==? 3KC1 + 15IC1 + 9H2O (2)

by addition of equations 1 and 2 and dividing by 5 we get:

KIO, + 2KI + 6HC1 ?=± 3KC1 + 3IC1 + 3H00 (3)

Therefore a solution of concentration 33 mM with respect to IC1

(i .e . 5.35 mg of ICl/ml which is equivalent to 4.18 mg of f per

millileter) can be prepared by dissolving 166 mg of KI in 8 ml of 6M

HC1, to this added by forcible injection to avoid precipitation of I_ -

107 mg of KIO3 dissolved in 2 ml of H2O then completed to a total

volume of 40 ml H-O. The resulting solution was shaken twice by 5 ml

CC1. aliquot to extract any I™ free in the solution. The aquous layer

was then aerated for one hour by bubbling moist air through it and the

volume is finally made up to 45 ml. The purity of the solution was

controlled by measuring the absorbtion peak at 460 nm wave length on

spectrophotometer LKB 4050 UV/visible apparatus (85) (86).

Since high Cl concentration stabilizes IC1(3) the solution was

diluted with 9 vol of more than 2 M NaCl before use .

Since only radioactivity that is in the IC1 form takes part in

substitution or addition reaction, iodine monochloride must be of high

specific activity. Iodine monochloride can be made radioactive through

125either i) isotopic exchange reaction between radioactive I and the

125 125inactive IC1, and in this case the fraction of I present as IC1depends on the relative masses of the exchanging forms : (87)

125or (ii) through the direct preparation of IC1 according to reaction

125number (3) using radioactive Na I prepared by oxidizing the total125iodine in the carrier free Na I solution with addition of iodate to the

stiochiometric amount of Nal.

2.2 Labelling of Oil with Iodine Monochloride (ICl) Method :

a) Cold (inactive) labelling : -

In order to know the feasibility of labelling the oil using ICl, some

experiments were carried out by using prepared inactive ICl and

following the labelling process spectrophotometrically.

The characteristic peaks for iodide, oleic acid, olive oil and

iodine monochloride as well as ICl-oil dissolved in the solvent-

(petroleum ether, diethyl ether and acetic acid, 70,30,1.5 V V V ) were

recognized by scanning on the UV-visible UNICAM sp 820 series 2 in

order to identify any change in the absorption peaks and the intensity

at every peak. The results are given in figures 6 - 1 6 and table 11.

Olive oil was labelled using inactive laboratory prepared ICl. The

ICl was prepared in the following manner :

b) Preparation of (ICl) for labelling :-

In a separating funnel 0.045 mM potassium iodide (11.25 ml), 0.21

mM potassium iodate 3.75 ml and 8 ml saturated solution of sodium

TABLE 11 : THE ULTRA VIOLET SPECTRUM STUDIES FORLABELLING OF OLIVE OIL BY INACTIVE ICL

System Peak in my ( O p t i c a lDens i t y ) Comment

0.1 M Nal ,inSolvent 1A"

251 (1.56), 257(1.66) and

l - " > Figure (7)

3 peaks characterist icof Nal

2% Oleic acidin 1A';

246 (1.52), 250(1.5), 256(1.26), 266(1.52)

Figure (12)

The four peaks arecharacter ist ic of oleicacid 246, 250, 256, and266

1% Oleic acidin 1A* + traceNal

21*5(1.26), 250(1.46),256(1.20) and 267(1.30)

Figure (14)

Small decrease at allpeaks

2% Oleic acidin 1A'r+ traceNal + 2g si 1icagel

246(1.22), 250(1.34),256(1.01), and 266 (1.18)

Figure (13)

Small decrease at allpeaks.

2% Olive oil in 245(1.28), 251(1.54),1A* 257(1-50), and 267(1.8)

Figure (9)

Four peaks characteristicof olive orl 245, 251,257, and 267

2% 01ive oilin 1A: +trace Nal

246(1.24), 250(1.44),257(1.38), and 267(1.66)

Figure (11)

Small decrease at allpeaks

2% Olive oilin 1AV + traceNal + 2 gsi 1ica gel

245(1-24), 250(1.48),257(1.44), and 267(1.74)

Figure (10)

I, ( 0.39)mM 245(1.18), 250(1.44), 2572 (1.38), 262(1.24)in 1A- Figure (6)

1A = Petroleum ether, Diethyl ether, Acetic acid. 70: 30 : 1.5, V:V:V

Continued

Table 11 (Continued)

46

System Peak in my ( O p t i c a lDens i t y )

Comments

IC1(Prepared)0.39mM in 1A

245(1.2), 250(1.54), 257(1.54),and 263(1.42)

Figure (8)

in

12h, 24h

277(1.4), 271(1.36)

(15)

Two

characteristicof ^belled

0.39mM IC10.3 ml OliveOil in 1A +3 g Si 1icagel after1h, 12, 24h

277(0.8), 270 (0.76)

Figure (16)

There is adecrease ata l l peaks

ISO J'S

Uaveiength (myO

Figure (6) : 0.39 mhl in [lA] [petroleum ether, Diethyl ether,

Acetic acid. 70 : 30 : 1.5. V:V:V]

JJ5 TSO

Wavelength (mju)

Figure (7) : 0.1 M Nal in [1A]

o

Wavelength (m/j)

Figure (8) : 0.39 mM ICl in [1A]

Figure (9) : 01ive o i l in 1A

oin

J« 730 J'S 300

wavelength (m^i)

Figure (10) : Ol ive o i l +t race Nal + s i l i c a gel in 1A

:>9 'so

Wavelength (m;u)

Figure (11) : O l ive o i l +- t race Nal in 1A

250 374

Wavelength (m_/i)

Figure (12) : Oleic acid in 1A

Figure (13) •: Oleic acid +trace Nal + silica gel in 1A

Figure {\k) : Oleic acid +trace Nal in 1A

50

ISO 37 : 3CO

Wavelength (mji)3 16

Time in hours

Figure (15) : Labelled oilive oil after a) 1h b) 12h c )

lit

Wavelength (mju)8 16

Time in hours

Figure (16) : Label led o l i v e o i l in the presence of s i l i c a gel

a f t e r a) 1h b) 12h c)

2 4

51

chloride, and 30 ml of (petroleum ether, diethyl ether and acetic

acid 70,30, 1.5 V/V/V) were then added. The whole content of the

funnel was shaken well and 5.0 mM hydrochloric acid (5 ml) was added.

The funnel snaked until the pink color of the iodine monochloride (ICl)

developed. The ICl was immediately separated in the organic layer and

used for labelling.

c) Labelling Procedure :-

In a 50 ml conical flask 0.39 mM of ICl 0.3 ml of olive oil are mixed

together. The flask contents were stirred by magnetic stirrer.

Labelling process was followed up through the spectroscopy method.

The results are demonstrated in figures 15, and 16.

2.3 . Iodine-125 monochloride method

a) Preparation of (125IC1):

In a separating funnel containing 0.0045 mM (1.125 ml) potassium

iodide, 0.021 mM (0.375 ml) potassium iodate and about 20 v Ci of

Na125I(74xl04Bq). 0.5 ml of saturated solution of sodium chloride and 3

ml of organic solvent were then added. The whole content of the

funnel was shaken well and 0.5 mM (0.5 ml) hydrochloric acid was

added. The funnel shaked untill the color of the radioactive iodine•I n c 125

monochloride ( I C l ) deveolped (table 12). The ICl was immediately

separated and used for labelling.

52

TABLE 12 : DISTRIBUTION COEFFICIENT OF 20 uCI

OF 125ICl AT ROOM TEMPERATURE

ORGANIC

SOLVENT

Benzene

Pe t ro l e r Ether

D. E. E.

n-Heptane

BETWEEN AQUOUS

LAYER

COLOR

Pink

Pink

Faint Yellow

Purple

LAYER AND ORGANIC

D I S T R I B U T I O N

C O E F F I C I E N T

41.38*

75*

Sk.k%

53

IOC

b) labelling Procedure with ("3IC1) :

In a 10 ml round bottom flask fitted with a condenser we put 0.039

125mM of IC1, 30 ul of olive oil (or oleic acid) and 3 ml of the organic

solvent and stirred by magnetic stirrer. Tap water was used as cooling

system in the condenser. A water bath was also used to adjust the

temperature at the required degree. The round bottom flask has an

opening with a septum for specimen handling by a syringe at different

periods of time to find out the labelling percentage. Each specimen

taken was 10 ul.

The percentage of labelling is shown in Figure (17) for olive oil and

in figure (18) for oleic acid in different solvents.

As it has been noticed that the labelling yield was changing from

one preparation to the other showing the great dependence of labelling

125on the method of IC1 preparation. This called for the use of

commercial iodine monochloride (IC1) instead of that prepared in the

laboratory. Figure (19) compares the labelling yield with IC1 prepared

in the laboratory and the commercial IC1 (purified and unpurified).

The purity of the commercial iodine monochloride (IC1) (Merck) was

tested to determine the percentage of free iodine (I , ) through the use

of sodium thiosulfate (75) (Na2S2O35H20). It was found that the

commercial iodine monochloride (IC1) used in this work contains 12% as

free iodine.

TO

• 0

• 0

40.

M

10

. . .

.jf—*"' * A- A—

/

A• a

B

A

C

a

A

®

10 90 SO 70 90 110 ISO ISO 170 190 210 230 250

Time in minutes

Figure (17 ) : Labelling of Olive oil with iodine monochloride (IC1)

A . in diethyl ether at 33°C

B. in petroleum ether at 5b°C

C. in n-heptane at 95°C

D. in benzene at 76°C

55

80 '

70

60

90

.-.40«*

•D

"5 30

20

10

-B- -a-

A-B- -a-

10 30 50 70 90 110 130 150 170 190 210 230 250

Time in minutes

Figure (i8) : Labelling of oleic acid with iodine monochioride (IC1)

A in diethyl ether at 33°C

B in petroleum ether at 56°C

C in n-heptane at 95°C

D in benzene at 76°C

56

6 0 -o-

so

40

30

20

10

1 0 3° 50 70 90 110 130 150 170 190 210 230 250

Time in minutes

Figure (19) : Labelling of oleic acid with iodine monochloride

( 1 2 5 . e i )

A = Commercial IC1 in benzene at 76°C

B = Purified commercial Id in benzene at 76°C

C = Prepared I C.I in benzene at 76°C

57

The commercial iodine monochloride was purified from the free iodine

using the solvent extraction by tb<j organic solvents CC1- and COEO.4 6 6

Table ( i j ) show the wavelength of maximum

absorption of I2 and IC1 in different solvents. Figure (20) shows the

wavelength of maximum absorption of IC1.

TABLE (13) : WAVE LENGTHS OF MAXIMUM ABSORPTION

IN DIFFERENT SOLVENTS

Species

Solvent

C 6 H 6

'2

X nm

519

501

297

Extinction

coefficient

900

1036

9767

IC1

Anm

1*60

<»35

287

Extinction

coefficient

160

220

9600 - 9000

10000

5000

1000300'

200 300

1}IC1 in CCl^2)I"I in *c en sens

400 500

Figure (20) : Wavelength of maximum absorpXion of IC1

59

2.4. Labelling of Olive Oil and Oleic acid with Chloramine-T (CAT):

a) Preparation of CAT Solution:

2 mg of CAT (Riedel-de Haen) was dissolved in 10 ml of acetone at

room temperature. The dissolved CAT was freshly prepared within 10

minutes of starting the experiment.

b) Labelling Procedure with CAT :

In a 10 ml round bottom flask fitted with a condenser we put 20P ci19> 4 191

of Na i ' !3I (74 x 10* Bq). The Na ^ I was dehydrated under vaccum.

3 ml of the organic solvent, 30 yl of olive oil (or oleic acid) and 5 pi of

CAT were then added and stirred by magnetic stirrer. Tap water was

used as a cooling system in the condenser. A water bath was also used

to adjust the temperature at the required degree. The round bottom

flask has an opening with a septum for specimen-handling by a syringe

at different periods of time to find out the labelling percentage. Each

specimen taken was 10 yl.

The labelling yield is shown in Figure (21) for olive oil and Figure

(22) for oleic acid.

2.5 Quality Control Systems:

Thin layer chromatography technique was used to determine the

60

3 O i

80 120 160 200

TIME IN MINUTES

240

F i a u r e (21) : Labe l l ing of O l i ve Oi l w i t i . (CAT)

A in n-heptane a t 95°C

B in methy l -n-propy l -ketone a t 7OCC

C in benzene a t 76CC

D in acetone a t *i5°C

61

80 120 16 200Time in minutes

240

Figure (22) : Labelling of oleic acid with (CAT)

A in n-heptane at 95°C

B in methyl-n-propyl-ketone at 70°C

C in benzene at 76CC

D in acetone at i»5°C

62

quality of labelling. Infrared spectrophotometry was used to determine

the location of labelling.

In the following a review on chromatographic methods is given.

2.5.a Thin-layer Chromatography Technique (TLC) :

A good deal of work has been carried out on fatty acids analysis by

TLC. In the following paragraphs a review of some aspects of this

work is given.

Sgoutas and Kumnerow (76) have studied the methyl

polybromostearates corresponding to oleic, linoleic and linolenic acids.

They used a thin layer (250-275y ) of silica gel on glass (20x20 cm), a

mixture of 96 vol. of Skely solvent B (bp67-68°C) and 4 vol. of

anhydrous ether served as the developing system for the separation of

the bromo-derivatives.

The results of R- values of brominated methyl esters of fatty acids

were (0.78, 0.75 and 0.73) for methyl oleate, methyl linoleate and

methyl linolenate respectively.

Tuna, et al.(52) reported the radioiodenation of olive oil and oleic

acid. They used a glass plate (20 x 20 cm) which has been coated with

a thin layer of silica gel. The developing system, they

63

used was a mixture of petroleum hydrocarbon (b.p. 60-70°C), diethyl

ether and glacial acetic acid (70 : 30 : 2, V:V:V respectively).

The results of R,. values of olive oil and oleic acid were 0.6 and

0.44 respectively.

Robinson and Lee (57) studied the radioiodenation of fatty acid131( I-oleic acid). The radioiodenated fatty acid was determined by TLC

on cellulose acetate using 320:80:1 heptane, diethyl ether and acetic

acid as a solvent. They found that free iodide remained near the

origin whereas the fatty acid migrates with R,. value of 0.8 - 0.9.

Bevenue (77) outlined a note of thin-layer chromatographic exami-

nation of various seed oils. He used plastic sheets pre-coated with 0.1

mm of cellulose. The sheets were developed in glacial acetic acid.

This was less efficient in the separation of the various components of

the oil sample and less sensitive in detection by the iodine-starch

reaction. On the other hand, Bevenue (77) found that the sheets

which were coated with liquid paraffin and developed in glacial acetic

acid gave good distribution.

Beierwaltes, Shaw and Roy (78) studied the myocardial uptake of

labelled oleic and linoleic acids, the total triglycerides of olive oil. The

sample of olive oil was dissolved in petroleum ether (bp30-50°C) and

then silica gel plate (20 x 20 cm) of 0.5 mm layer thickness was

used. The plate was developed in petroleum ether (bp 30-50°C) diethyl

ether (99%) and formic acid (70:30:1.5, V:V:V). Bands were visualized

by spraying the plate with 2.7 dichloroflorescein in ethanol (0.1* YKV).

The band containing the total triglycerides ( R* s 0.85) was separated

off and exhaustively extracted with CHC1,. Radiochemical purity of

their products was ascertained with thin-layer chromatography using

silica gel with flourescein indicator and solvent system of petroleum

ether, diethyl ether and acetic acid (90:10:0.5, V:V:V). The labelled

products gave R*. of 0.44 for oleic acid and R,. of 0.36 for linoleic acid.

Damiani and Burini (79) reported the determination of the

triglyceride composition of olive oil by a multistep procedure to isolate

the total triglycerides of olive oil. The sample of olive oil was

dissolved in petroleum ether (bp 30-50°C) and then silica gel plate (20

x 20 cm) of 0.5 mm layer thickness was used. The plate was developed

in petroleum ether (bp 3O-5O°C) diethyl ether (99*) and formic acid

(70:30:1.5, V:V:V). Bands were visualized by spraying the plate with

2.7 dichloro-florescein in ethanol (0.1% W/V). The band containing the

total triglycerides (Rj. 0.85) was separated off and exhaustively

extracted with CHC1_.

At the beginning we used five systems to determine the Rf for the

olive oil, oleic ac\d and radioactive sodium iodide with carrier. Tables

(14, 15, 16) show our results for different three systems.

65

System 1 :

The eluent was petroleum ether, diethyl ether and 99 formic acid

(70:30:1.5, V:V:V). Table (14)

System 2 :

The eluent was n-hepatane, diethyl ether and acetic acid (320:80:2,

V:V:V). Table (15)

System 3 :

The eluent was methanol and HgO (85:15, V:V). Table (16).

System 4 :

The eleuent was 99 acetic acid. DC-plastic sheet coated with

cellulose 0.1 mm without florescent and glass plates coated with silica

gel 0.2 mm with floresint F2 5 4 were used. This system does not show a

clear distribution neither for olive oil nor for oleic acid.

System 5 :

The eluent was petroleum ether, diethyl ether and 99 acetic acid

(70:30:1.5, V:V:V). Glass plates coated with silica gel with flourescent

66

TABLE ( I t )

SYSTEM (1)

The eluent was petroleum e ther , diethyl ether and 99% formic acid (70:30:1.5, V:V:V)

De-Plastic sheetCellulose 0.1mm

Conroonent without flourescent

glass p la t i c ( s i l i cage l ) 0.2nun Aluminum Sheetcoated withs i l i cage l 0.2mm

F_,_. with flourescent

I2-Vapor D.C.F* I -Vapor U.V. D.C.F* I2-Vapor

Olive Rf = 1 Rf = 1 R- =0.37 R =0.45 Rf=l R,. =0.31Oil

Rf,=0.45 R f2=l Rf2=0.48

R f.=0.9+ R£3=0.69

Rf4= 1 + ' ' Rf4=1+

OleicAcid

Rf x = 1 Rf = 1 Rfl=0.16 R£1=0.41 Rf=0.62 Rf=l

Rf2=0.22 Rf2=0.69

Rf3=O.27+ Rf3=0.76

Rf4=0.81

v 125 TNa I Rf = 0. (activity}** Not (activity)Regular

Rf=0 (activity)

125 IC1 Rf = 0 (activity) Rf=0 (activity)

+ = wide band* = 1:0.05% ethanolic spray solution of 2,7-dichlorof lurescein. See Ref.** = Counted using a Beckmann gan.ma counter (5500).

67

TABLE (15) :SYSTEM (2)

The eluent was n-heptane, diethyl ether and acetic acid (320:80:2, V:V:V)

De-Plastic sheet glass paltic (silicagel) 0.2mm Aluminum sheetcoated withsilicagel 0.2mm

Cellulose ).lmm ¥ with flourescentComponent without flourescent

I2=Vapor D.C.F. I2=Vapor U.V. D.C.P

OliveOil

Rf - 1 R£1=0.

R£2=0.

Rf3=0.

R f 4=o.

9

1

16

19

Rfl=0.

R£2=0.

Rf3=0.

1 D — r

14

54

1.51 R£1=0

Rf2=0

Rf3 = 0

Rf4=°

.55

.9

.14

.16

R£5=0.49

Oleicacid

R- = 0.81 Rfl=0.14 R£=0.39 R£=0.31 Rfl=0.38

R£2=0.47 R£2=0.86

Na 1 2 5Iwithcarrier

R£ = 0 (activity) Rf=0 (activity) Rf=0 (activity)

125ICl Rf=0 (activity) R£=0 (activity) R£=0 (activity)

( + = wide band )

68

TABLE (16) :SYSTEM (3) :

The eluent was Methanol : H20 (8S:IS, V:V)

DC-Plastic sheet glass platic (silicagel) 0.2mm Aluminum sheetCellulose 0.1mm F_5. with flourescent coated with

Component without flourescent silicagel 0.2mm

I2-Vapor D.C.F 12-Vapor U.V. D.C.F. I2~Vapor

Olive Rf = 0+ Rf = 0 Rf=0

+ Rf=0+ Rf=0

+ R-=0+

Oil t

Oleic Rf = Rf=0.49 Rf= Rf=0.52+ Rf=0.48

+ Rf=0.65+

acid 0.17-0.96+ 0.4-0.9+

Na 125I Rf = 1 Rf = 1 R, = 1withcarrier

1 IC1 Rf = 1 (activity) Rf = 1 (activity) Rf=l (activity)

( + = wide band)

^254 w a s usec*" "^^s s v s t e m gave Rf f° r olive oil as follows:

R f l = 1> Rf2 = ° ' 2 9 a n d B 3 = ° ' 2 5

Of these five tested systems, the second system was chosen for use

during our work becuase it gave good distribution and the radioactive

material remains at the origin. The plastic plates coated with cellulose

(0.1 mm) (Merk) was used during our study because it is easy to cut

when we want to count the radioactivity.

2.5-b IR-Spectrum :

In the IR-spectrum study for both olive oil (figure 23) and oleic

acid (figure 25), the unsaturated bond was demonstrated at a wave

number of 1400-1500 cm" . This un

bi-peak (a? shown in the two figures).

number of 1400-1500 cm . This unsaturated bond is shown as a

In order to know the effect of temperature change on the

IR-spectrum for both olive oil and oleic acid, temperature was raised

up to 90°C for 2h. The IR-spectrum was, then taken but no change

has been noticed as it is cleared out from figure (24) and figure (26).

To study the effect of iodine (I~) on the double bond, two organic

solvents were used which are benzene (C-H«) and carbon tetrachlorideb b

(CC1.). IR-spectra for iodine 0.1 M in benzene and carbon tetra-

70

chloride are shown in figure (27) and figure (28) respectively. The

spectra for oleic acid dissolved in benzene and carbon tetrachloride are

shown in figure (29) and figure (31) respectively. 0.2 mM of iodine

were then added to the oleic acid dissolved in benzene and to the oleic

acid dissolved in carbon tetrachloride. The temperature was raised

up to 35°C with continuous stirring for 2 h. The spectra for these are

shown in figure (30) and figure (32) respectively. It is found that

presence of iodine causes some change in the spectrum, especially, on

the bi-peak at a wave number of 1400-1500 cm" which represents the

double bond. This gives an evidence that iodine has caused some

change in the double bond. In fact we have to study this point in

depth in order to identify the exact change in the double bond.

Lastly, the spectrum of oleic acid labelled with Kl was taken. It

was noticed that some change has already happened in the bi-peak at

the wave number of 1400-1500 Cm"1 . This change is demonstrated in

figure (33).

71

Uavenumber cm"

Figure (23) : 01ive oi 1

Wavenumber cm-1

Figure [2k) : Olive oil heated at 90°C for 2 hours

72

Uavenumber cm

Figure (25) : Ole ic ac id

Uaveniimber cm-1

Figure (26) Oleic acid heated at 9O°C for 2 hours

73

- Wavenuniber cm-1

Figure (27) : 0 .1 M I in benzene

Uavenumber cm

Figure (28) : 0.1M

-1

Wavenuniber cm"

Figure (29) Oleic acid dissolved in benzene

Wavenuniber cm"1

Figure (30) : Labelling of Oleic acid with I in benzene

75

Wavenumher cm" '

Figure (31) : Oliec acid dissolved in CC1,

Wavenumber cm

Figure (32) : Labelling of Oleic acid with

76

MOO 1400

Wavenumber cm-1BOO

F i g u r e (33) : L a b e l l i n g of O l e i c a c i d w i t h IC1

CHAPTER 3 : DISCUSSION and CONCLUSIONS

3.1 Labelling of Olive Oil and Oliec Acid withIodine Monochloride Method.

3.2 Labelling of Olive Oil and Oliec Acid with Chlor-amine-T Method.

78

CHAPTER 3 : DISCUSSION AND CONCLUSIONS

3.1. Labelling of Olive Oil and Oleic Add with Iodine Monochloride

(IC1):

Iodine monochloride (IC1) was discovered by Davy and Gay-lassac

(83).Greenbaum used iodine monochloride (IC1) for the iodination of oils

since 1937 (84). In 1967 Helmkamp (85, 86) used (IC1) for

131

I-labelling of proteins.

The chemical forms of iodine species that react with fatty acids

using (IC1) has so far not been identified unequivocally (87). In this

work for labelling of olive oil and oleic acid using (IC1), an inactive

prepared (IC1) was firstly used and the labelling process was followed

up through the U.V. spectrum. Ultra-violet absorption peaks of !„,

IC1, Nal, oleic acid and olive oil dissolved in [Petroleum ether, diethyl

ether, acetic acid, (70:30:1.5, V:V:V)] [1A] and measured against the

same solvent as blank were identified. As a result of the Ultra-violet

spectrophotometric studies for the different chemicals used, table (11)

and figures (6-14) illustrate that there are three absorption peaks at

wave lengths of 251, 257, 246 m y for Nal, four absorption peaks at

wave lengths of 245, 250, 257, 262 m y for I , , four absorption peaks

at wave lengths of 245, 250, 257, 263 m y for IC1, four absorption

peaks at wave lengths of 246, 250, 256, 266 my for oleic acid and four

absorption peaks at wave lengths of 245, 251, 257, 267 my for olive oil.

From these results it appears that we can rely on absorption peak

at 266-267 millimicrons to recognise the oil in presence of Nal since this

79

peak does not appear in Nal spectrum. The addition of silica gel,

figures (10, 13, 16) show that it absorbs not only oleic acid and olive

oil but also the labelled olive oil indicating that one can not use silica

gel for purification of the oil from other species.

When IC1 was added to olive oil two new absorption peaks at 271

and 277 my appear which differ from those peaks of both IC1 and/or

olive oil. This is an evidence of a new product formation which is

iodinated labelled olive oil. The change in absorbancy of this peak with

time (lh, 12h, 24h) shows that the maximum labelling took place after

one hour and that labelling decreases with time indicating the

unstability of labelled olive oil. This unstability may be attributed to

chemical damage caused by the high concentrations of iodinating

reagents used and/or by impurities that may be present in iodide

solutions or as a result of alteration of the structure of the oil (88).

Radio-active laboratory prepared IC1 was then used with benzene

(at 76°C), petroleum ether (at 56°C), diethyl ether (at 33°C) and

n-heptane (at 95°C) as solvents. The highest yield was obtained

through using diethyl ether. The yield was more than 80! for oleic

acid and more than 10% for olive oil after 15 minutes. The labelling

yield of oleic acid in petroleum ether increased with the increase of time

reaching a maximum percentage of 62% after 120 minutes. In case of

n-heptane, labelling yield was found to reach maximum value of 63%

after 5 minutes then decreased sharply to 40$ at 100 minutes period.

80

This decrease may be attributed to the fact that the C-I bond

(238 KJ mol ) (91) is relatively weak compared with the C-H bond

(412 KJ mol" )(91) and it is therefore not surprising, with increase of

temperature (95°C) and long reaction time, that one of the main

impurities formed in self-decomposition of iodine labelled compounds is

inorganic iodine (92). Benzene shows the lowest labelling yield of 25%

although at the beginning the percentage of labelling increases from 5%

at 5 minutes to reach a maximum value of 43% after 60 minutes.

In case of olive oil, the case is approximately the same where the

highest labelling was achieved when using diethyl ether. In petroleum

ether the same trend in labelling was noticed, where labelling increase

with the increase of time reaching stable value of 35% at 55 minutes

period. The same trend was noticed in case of benzene and n-heptane.

However in case of olive oil the labelling yield was lower in benzene

than in heptane a case which is the same as what had happened in

oleic acid.

The lower labelling yield in case of olive oil may be attributed to

the fact that olive oil used in this work contains only 58.12% as oleic

acid, and 13.69% as linoleic acid i.e. approximately 71% of the olive oil

is found as unsaturated fatty acids, a case which indicates again that

labelling took place in the double bond which is in good agreemnt with

other authors working on caster oil (89).

81

As benzene shows the lowest labelling percentage in case of oleic125acid curve it was chosen as the solvent for labelling using the I d

prepared from commercial I d . Figure (13) gives the percentage of125labelling of oleic acid using purified and unpurified I d . From this

125curve it appears that commercial IC1 gave a higher labelling yield125than that of I d prepared in the laboratory. 65% labelling yield was

reached in the first 15 minutes period in contrast to a yield of only 22%125for the prepared I d . The commercial IC1 purified from the other

iodine species, however gave only a yield of about 40% after 15 minutes.

This reduction in the yield in case of purified IC1 indicates that other

iodine species share in the labelling process. It appears that the

labelling takes place to some extent as a result of the persence of the

species I d , !„ , I, and IOH depending on the medium used (90).

51" + IO- + 6H+ ^ 3I2 + 3H2O

3I~ + 3H O + ?=* 3H0I +31,

3HOI + 3H+ + 3d" = £ 3IC1 + 3H2O

The IR-spectrum for Io added to the oleic acid in CC1. solvent^ 4

(figure 32) shows a change in the double bond indicating that I« also

labels the oil.

82

j Labelling of Olive Oil and Oleic Acid With Chloranrine-T(CAT)

The use of (CAT) is considered to be as one of the oxidation

uethods which was widely used in labelling experiments. Chloramines

> iBve been used in the past for the generation of IC1 to iodinate anilides

as well as phenol, naphthol, and aromatic ethers (87).

if

: IC1 is obtained in acidic medium by the reactionVN-C1+2HI = ^N-H+HC1+I2

The HC1 reacts with another molecule of chloramine, liberating

f- chlorine, which combines with iodine to yield I d .

H Hunter (80, 81) used this method for studying the labelling of

J, proteins with iodine.

f-

; Krohn (82) used the same system for studying the possibility of

labelling fibrinogen with radioiodine.

The commercially available chloramine-T is the sodium salt of

Pl-chloro-p-toluene-sulfon-amide] the formula of which is shown below:

CH.

A s is generally known electronegativity is a property which

indicates that an atom tends to attract an electron. Since chlorine is

I

83

more electronegative than iodine, the former can be used to remove an

electron from iodide. As the result of this electron transfer, chlorine

is converted to chloride and iodide converted to "cationic iodine" i.e.

iodine in the +1 valency state (87).

If such an electron transfer system is operated in the presence of a

fatty acid, the electron depleted iodine (I ) will react with the fatty

acid.

In this work studies were carried out aiming at using CAT method

for labelling olive oil as well as oleic acid in the organic solvents

n-hepatane, benzene, acetone and methyl n-butyl ketone (MnPK) at a

temperature just below the boiling point of each solvent. Figures (21,

22) show the results obtained with oleic acid and olive oil. The

labelling yield reaches a maximum value of 50% after 200 minutes in case

of oleic acid while it is only 28% in case of olive oil, in case of the

solvents benzen and MnPK the yield is low for both oleic and olive oil.

The low yield in case of olive oil may be explained in view that olive oil

contains only 58.12% as oleic acid. (71)

While the general trend for both oils was che increase of labelling

with time yet it was found that in case of acetone the labelling yield

decrease with time. This decrease may be attributed to some extent to

the high solubility of CAT in acetone, which compete with the oil for

the iodine (87). Also this low labelling may be as result of low

temperture

(4F°C) in case of acetone which means low release of CAT from the

acstone. In accordance with Greenwood (138) there appears to be a

critical amount of the reagent (CAT) below which labelling is

i isignificant. Bocci (139) reported that an inverse relationship exists

Vetween reaction time and the amount of oxidant used, which may

explain the low yield in case of acetone as a result of low oxidant

concentration available.

CHAPTER 4 : LABELLING OF OIL WITH 9 9 mTc

4.1 Introduction.

4.1.1 Generator Fundamentals.

4.1.2 Technetium-99m Milking System.

4.1.3 Methods for Separation of " T C .

4.1.4 Comparison of ^Tc Generator Forms.

4.1.5 Use of 9 9 mTc in Labelling.

4.2 Experimental and Results.

4.2.1 Preparation and Control of 9 inTe.

4.2.2 Determination of Radiocontaminants in Old ^ T c Generators.

4.2.3 Quality Control by Thin Layer Chromatography and PaperChromatography.

4.2.4 Labelling of OKve Oil by 9 9 mTc.

4.2.5 Labelling of Olive Oil by Reduced 9 9 m Tc.

86

CHAPTER 4 : TECHNETIUM

4.1 Introduction :

Severs! short-lived radioisotopes which are useful in clinical

radioisotope work are the daughters of longer-lived parents. It is thus

possible to perpare a generator or "cow" containing the parent

radioisotope from which the daughter can be "milked" whenever it is

needed. Table (2) gives details of a number of these parent daughter

systems.

4.1.1 Generator Fundamentals (96) :

Milking systems are well known for a long time (97). The most

important factor in these systems is the establishment of transient

equilibrium between the parent and its daughter isotope. The parent

99isotope Mo ( t 1 / 9=66.7h) which is freshly purified from its daughter

99m 99products ( Tc + Tc) will continue to generate technetium isotopes

99as a result of beta decay of Mo (98).

From the laws governing the transient equilibrium (3, 4), the99 99m

maximum total activity of the mixture ( M o + Tc) will be reached at

time (t ) given by :

87

XTc 'XMo 2 XMo XTc " XMo

99 99m

which is 17 hours in case of Mo + Tc mixture. The generatedmTc reaches its maximum activity at a time "t"" independant of the

counter detection efficiency given by :

t - = * ta T c

m XTc ~ AMo XMo

This time is 22.91 hours for technetium-99m. On the above

mentioned bases the changes of activities in a generator with time is99given in table (17) and in figure (34) (for s 886 mCi Mo produced

as a result of irradiation of 25 gin MoO_ at thermal neutron flux ofo

13 210 n'cm . s for saturation).

88

TABLE (17) : CHANGE OF ACTIVITIES WITH TIME IN

A 100mCi99Mo GENERATOR (Ref. 96)

Generatoractivity

mCi

100

78

60.8

A7.5

37

29>22.5

17.6

13.7

10.7

8.3

Generator age(from time of dispatch day)

Zero

1

2

3

k

5

6

7

8

9

10

9 9 l\c Activitymi Iked* perstage mCi

di spatched

62. k

kB.6

38

29.6

23.2

18

14.1

11

8.6

8.6

89

1024 48 72 96

TIKE (HOURS)

120 144

Figure (3*0 : Theoretical Growth and Decay of99mTc in Pure Parent 99Mo. (96)

90

When the transient radioactive equilibrium is established, the

activity of the generated technetium is 1.098 greater than that of the

99parent Mo considering equal detection efficiency.

The nuclear properties of 99m-technetium isotope are shown in

99 99table (18). The decay sequences of the parent isotope Mo to Ruare as follows (100):

8

x 10py)

99

The decay shceme of Tc (101) as well as 'is parent isotope

JVIo are given in figure (35 and 36).

TABLE ( 1 8 ) : NUCLEAR DATA FOR TECHNETIUM

Isotope

" m T c 6.0h9 9Tc

( 99Tc h a l f - l i f e

2.12 X 105yr,

B to 99Ru

Mode of decay,Energy (Number/100disintegrations)

Isometric t rans i t ion

y-rays from Tc

0.0022 (98.6)

0.U05 (98.6)

0.U27 (I.**)

Method ofProducing Isotope

Parent/daughter system

99M Q 67hr 99mTc

99 6 "Mo produced by reactor

i r rad ia t ion of 5 V > (23-75S

or by separation from

f iss ion products.

0.142 McV-

0.140 .McV-

0.0

"•Tr

98.6% 7. (Internalconversion ratio = 0.005)

i "Tr ( T | = 2. I X 10'vr)

__"Ru (Stable)

-»,= O.OOi McV7 : = 0. HO McV1 i = 0 . H 2 McV

Figure (35) : The decay scheme of Tc .

Molybdenum-99Btla-minui decay

91

1

\

n0

1 00*?1

;

0 9208

0 67U

C 5090

rt o igio

9 l\ 0 I4Z6

F i g u r e (36) : The decay scheme o f99

Mo

92

Advantages and Disadvantages in Selecting "'Tc for medical use:

Technetium-99m was selected for use in nuclear medicine because

of many advantages it has. These advantages are that the -y-ray

energy of 140 KeV is ideally suited for the Anger Camei'a. It gives

excellent resolution and efficiency with a low energy collimator; raTc

does not have a primary particle emission and its low internal

conversion of its 140 KeV y-ray and its 6h half-life allow the use of

large quantities of the radionuclide with low i*adiation dose to the

99patient. The parent Mo has a 66.7h half life period which allows time

for shipment from manufacturer to hospitals, and finally the 6h half-life

of mTc allows rapid buildup of activity permitting frequent milking of

the generator.

On the other hand, Tc has some disadvantages which are that

99the 66.7h half-life of the Mo requires that the generator be replaced

weekly and requires shipment by air to distant places from the

manufacturer. The low y r a y energy of 140 KeV does not make it

ideally suited to detect deep-seated lesions in the body, the short

half-life of 6h is a disadvantage when delayed scanning procedures are

required and the chemistry of technetium is not well known and the

multiple oxidation states make it difficult to label certain compounds or

reagents (102).

93

-:." % ~ ,1-tinetfaim - 99m MiHring System:

In the preparation of any milking system, one of the important

factors is the purity and specific activity of the parent isotope. In99technetium generator, the parent isotope is Molybdenum-99, ( Mo).

99The specific activity as well as the purity of the Mo depends on the

way by which it is prepared.

Molybdenum-99 can be prepared in a nuclear reactor by:

a) Irradiation of natural molybdenum target mainly the oxide (MoO»)QQ QQ

according to the nuclear reaction: Mo (n, y ) Mo.

The radioactive (96) contaminants that may appear as side nuclear

reactions are given in table (19). Zirconium and Niobium isotopes are

the main contaminants, depending on irradiation time, cooling time and

the neutron flux. Molybdenum-99 produced by this way is of low

specific activity.

TABLE (19) : RADIOACTIVE ISOTOPES PRODUCED ON

IRRADIATING STABLE MOLYBDENUM IN

NUCLEAR REACTOR

Sk

Nuclear

Nuclide

92MO

Mo

95MO

96Mo

97Mo

98Mo

1 0 0MO

IReaction

Abundance

15.9

9-1

15-7

16.5

3.k

23.8

9.6

Isotope t.

93Mo 2 y

93mMo 7 h

99Mo 67 h

101Mo 15m

n,PIsotope

92mNb10

92Nb 10:

9\lb2.7

95Nb 35

96Nb 23

97Nb 72

1

ti

d

,o\

d

h

m

n ,a

1sotope

89Zr 97

93Zx9-5

95Zr 65

97Zr 17

t.

h

D5y

d

h

n . 2n, or

1sotope tJ

91Mo 15.5m

91mMo65 s

93 S 93mMo

Mo 67 h

See Ref. (96)

95

98b) Irradiation of molybdenum enriched in Mo by thermal

neutrons. In order to increase the specific activity and decrease to

some extent the radioimpurities, targets enriched upto 90 % in

molybdenum of mass 98 are irradiated in the neutron flux of a reactor.

The Molybdenum -99 produced by this way is of high specific activity.

However the price of enriched material is of high cost. To overcome

the expensive enriched targets some authors reported the use of recoil

techniques (96) on natural molybdenum materials or by transferring the

molybdate to the complexed chemical form phosphomolybdate.

oQg 238c) Irradiation of U or U targets in a stream of neutrons

235where molybdenum-99 is produced as result of fission U (n, fission)

Mo. The molybdenum-99 produced by this way is of very high99specific activity, may be carrier free. Fission-product Mo demands

elaborate and expensive processing facilities, and extreme care to avoid

contaminating the product with over fission products and the

highly-toxic a-emitting transuranic radionuclides. Despite the high

235 99

fission cross section of U and the high fission yield of Mo the

overall yield has to be restricted because of such practical

considerations as the ability to dissipate nuclear heat or to dispose of99highly radioactive waste. The specific activity of fission-produced Mo

is high ( >104 Cig"1). (3 , 95, 96)

The criteria for choosing the method of Mo production must

include economic, resources, and mode of utilisation. The practical

99difficulties associated with the production of fission Mo ore reflected

in the costs even in large-scale manufacture, the cost of producing 1 Ci

99of fission Mo may be upwards of four times of the cost of 1 Ci ofQQ

9 Mo(n, Y ) Mo. Besides the need to process highly radioactive

irradiated uranium in a manner which does not compromise the safety of

the environment, an infrastructure is required to deal with the special

problems of quality control and waste disposal.(4,95)

4.1.3 Methods for Separation of 99mTc :

99 99m

After preparing Mo (the parent isotope of Tc) by any one of

the last mentioned methods and geting it in its very high radiochemical

purity, begins the step of choosing the way by which Tc can be

milked out to receive the required amount of Tc. In the literature

three main methods are reported; 1) chromatography, 2) solvent

extraction, and 3) sublimation methods. A brief account of each method

is given below:

1) Chromatographic Method :

In this method molybdenum-99 in the molybdate or phosphomolybdate

form (96, 97) is retained on some sort of solid sorbing material as

alumina (100, 103, 104), hydrous zirconum oxide (105), manganese

dioxide (102) silica gel (106) or active charcoal (107). 9 9 mTc is milked

*nenever required by appropriate eluant for example isotonic saline

97

lution (0.9fcNacl solution) (96), acid solution of methyl ethyl ketone

5vol*0.01 M HC1) (105), 0.1 M HNO3 (102) or acetone (106).

2. Solvent Extraction Method :

In this method A"C is extracted by some organic solvent for

example methyl ethyl ketone (MEK) (108, 109, 110, 111), isobutyl

•ethyl ketone (112), bis-(2-ethyl-hexyl) phosphoric acid (113) and

pyridine derivatives (114, 115), then transferred to the required

•edium (105, 106, 107, 108) for application.

3. Sublimation Method :

In this method mTc is separated from its parent by sublimation of

the irradiated molybdenum target depending on the different volatilities

of their oxides (115).

*•*•* Comparison of 9mTc Generator Forms (104):

The choice of a particular generator system is usually made for

•chnical, economic and logistic reasons, with emphasis on one or other

these factors depending upon the circumstances.

This brief idea about the more common mTc-generator systemsws that the ideal generator has yet to be invented; all the current

98

i¥ersions have at least one disadvantage will- •' ' i : n d s t o l i m i t t h e i r

practical appl icat ion. The following i . i l - l - " ' < " l t a I n t h e advantages,

disadvantages and prospects of each

|. Chromatographic generator containing

natural molybdenum :

in ing <«. I > " M o P roduced from

Advantages

* Simple processina

* Only inexpensivelow specificac t iv i ty99

Mo requi red.

* Yield not 1imitedby extensivewaste disposalproblems.

* Simple to operateand portable.

* 99m_Tc separated

with high efficie-cy

Disadvant.vi"^

* Large size a Icolumn requ ii"for specific

99activity Mo.

" Low elutionProfile.elute volume.

Prospects

Development ofsubstrates otherthan aluminarequired toreduce thedimensions ofthe generator.

2. Chromatographic generator containing (n,y )98from enriched Mo.:

99

99Mo produced

Advantages Disadvantages Prospects

* Simple processing.

* Easy to operate andportable

* 99mTc separated withhigh efficiency.

* Elution profileimproved.

* Expensive targetmaterial and a veryhigh flux reactorrequired formaximum effort;probably the most

expensive method of

producing regq

unless the Mo isrecyc1ed.

Obsolesence

993. Chromatographic generator containing fission produced Mo

Advantages Oi sadvantages Prospects

-Use of physically smallgenerators permittedbecause of carrier-freecharacteristics of99Mo, giving not only

maximum radioactive

Tc but also reducedshielding mass.

* Simple, to operate andportable.

* Tc separated withhigh efficiency.

* Excellent elutionprofile.

* High capital cost ofprocessing plant;special problemsarising from gaseousfission products andsubsequent environ-mental hazards.

* Elaborate processingprecautions requiredto avoid fissionproduct or trans-uranic contamination

of 99Mo.

* Porblem of disposal ofother fission products.

QOm* High cost per mg Tc.

* Although atpresent this typeof generator iswidely used, itsinherent disadvan-tages are promptinga search foralternatives. Itis predictedtherefore, thatthe fissionqproduced "9Mogenerator wi11eventually besuperceded byadvanced designsincorporating

(n,Y ) 99Mo.

100

The sublimation generator containing (n,Y)Natural molybdenum :

99Mo produced from

D i sadvan tages Prospects

• Only inexpensive low-: Specific act iv i ty 99Mo

requi red•

• Ho chemical processing.

• Capable of being scaledupto Kci quantities.

• Product free fromchemical impurities.

• Very high radioactiveconcentrations easilyattained.

• High radionuclidicpurity.

• Low cost per Mg Tc.

* Version suitable foruse in small nuclearmedicine laboratoriesyet to be developed.

* Separation efficiencyreduced (25 - 50%)and speciallyprogrammed processcycles required toprevent even furtherefficiency deterioration.

DespiteabiIityproduce

itsto

ofexceptional lyhigh quality ,i t can not befully exploiteduntil itsquanti tativeperformancecharacteristicshave beenimproved.

Furtherdevelopmenti s requ i red.

5. The solvent extraction generator containing (n, y )from natural molybdenum :

99,Mo produced

Advan tages D i sadvan tages Prospects

* Only inexpensive lowspecific activity99Mo required.

* Capable of beingscaled up or down toindividual requirements.

High radioactiveconcentration99rn . L,

Tc attainable.

* High radionuclidicPurity.

High separation efficiency

* Low cost per mg 9 9 mTc.

" Apparatus complicated;highly trainedpersonnel required.

* Possible fire hazardwith MEK vapour.

* Possible interferenceby polymeric organic

residues in the 9 9 mTcproduct solution withsubsequent taggingreactions to produceundesirable changes inbiological properties.

Limited onlyif the problemof organicresidues, whichhas brought thismethod intodisrepute, isnot resolved.

101

t s i » of " " T c in Labelling :

The chemical form of mTc milked from the Mo-generator is in the

nertechnetate form TcO~. Chemically, mTcO^ is a rather nonreactive

species and does not label any compound by direct addition. In

labelling by technetium mTc, prior reduction of mTc from the

7+state to a lower valence state (3 +, 4+, or 5+) is required. Various

reducing systems that have been used are Stannous chloride (SnCL

2Ho0) (111). Stannous tartrate (112) ascorbic acid plus ferric chloride

(111), concentrated HC1, (113) sodium borohydride (NaBH4)(lll) and

ferrus sulfate (111). Among these Stennous chloride is the most

commonly used reducing agent in an acidic medium. It is used in most

preparations of mTc labelled compounds. Another method of reduction

of mTc 7+ involves the electrolysis of a mixture of sodium

pertechnetate and the compound to be labelled using an anode of

zirconium (113).

There are many compounds labelled by mTc; some of these

compounds are shown in table (20).

102

TABLE (20) : COMPOUNDS LABELLED BY " mTc

COMPOUND

# Human serum albumen

• Red cell hemoglobin

• Plasmin

* Dimercaposuccinicacid (DMS)

* Fatty Acids

* Oleic Acid

Gentamin

APPLICATION

Nuclear medicine

Nuclear medicine

Medical scintigraphy

investigations of99mTc-DMS biochemicalbehaviour in kidneytissue.

Nuclear medicine

Nuclear medicine

Scintigraphicstudies

Auther

Steigman J. (117)

Dewanjee, M. K. (118}

Sundrehagen, E. (ilV

Razumenic, N. (13^)

Oiengott, D. (115)

Moore, G. et al(119)

Ozker, K. (l16)

a n d R e s u l t s :

i this part of study investigations were carried out aiming at

olive oil with mTc. Since there are no stable technetium

s, and since mTc isotope used is a carrier free, a case in

we are obliged to use only radioactivity counting techniques. The

fhbelling technique used consists of mixing the oil in diethyl ether or

with the mTc in the same solvent with or without the reducing

- SnCl2 - then mixing thoroughly using a magnetic stirrer at

temperature for a known time, after which samples were taken and

chroniatographed to know the labelling yield. The chromatographic

technique used was ascending paper chromatography with 85% methanol

as developing solution.

Materials Used:

- Olive oil (Winlab Limited)

- Methanol (Analar Merk)

- Diethyl Ether (Analar Merk)

- Acetone (Analar BDH)

- SnCl2 . 2H2O (BDH)

- HC1 (Analar (BDH)

Tc kindly supplied by the Nuclear Medicine Department of

King Khalid University Hospital (KKUH).

- Four out of use Mo - mTc generator (Amersham type) kindly

supplied by Nuclear Medicine Department of King Khalid

University Hospital (KKUH).

(These have been used to determine the radiocontaminants within

the generator and also as a supply (from new ones) of the parent99isotope Mo)

- Silica gel plastic sheets 60 F 2 5- 0.2 mm (Merk)

- Cellulose plastic roll 0.1 mm (Merk)

- Whatman paper lm (Whatman)

4.2.1 Preparation and Control of 99mTc :

Molybdenum-99 fission product obtained as a result of eluting a

Tc generator by (1.5 ml, 1.5M) NaOH solution. The acidity of the

molybdenum solution was adjusted to be 0.1 M in HCl and 0.001 M with

respect to Molybdenum then absorbed on a column (8 cm long and 1 cm

wide) containing 5 g alumina (A1OO, for chrom&tography). The column

was washed thoroughly with 0.9% Nacl solution until no more activity

was detected in the washings and, also, until no more blue colour

appears when drops of the washings were contacted with stannous

chloride solution. The column was left for 24 hours after which the

daughter 9 9 m Tc was milked.

105

99m,Tc was e lu ted b y us ing 5-10 ml isotonic saline solution. The

Y-spectrum of the eluted m T c was measured a n d plotted on a

plot ter-pr inter ( t y p e Dataproducts) connected to a multichannel analyzer

(type 35 plus Canber ra ) us ing a well type 7.5 x 7.5 cm Nal (Tl)

crystal detector shielded with 5 cm lead and lined with 0.6 cm copper to

minimize in te r ference from lead X - r a y s . The MCA u s e d was equipped

with an iso-analyzer type 3543 s t a n d a r d l ibrary (Table 21) . However

since this l i b ra ry does not contain any technetium or molybdenum

60isotopes the MCA was calibrated using Co lines (1173 KeV), (1330

KeV), 137Cs line (662 KeV) and 85Sr (514 KeV). The linearity curve

is given on figure (37) showing that the first four channels have to be

neglected. Measuring the spectrum of Tc eluted shows its presence

at channel No.46 (No.42 after correction) indicating 140 KeV. The

Spectrum is shwon in figure (38) from which it appears that the

Tc milked is of very high radiochemical purity. The half-life curve

is shown in figure (39) indicating half-life period of 6 hours.

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Table 2 1Model 3543 Standard Library

80 ' 120 ' i£o ' 200 240 280 32"o 3&0

CHANNELS

Figure (37) : Lineari ty Curve

30 90 CHANNELS l5° 2I°Figure (38) : The gamma spectrum of Tc measured

MCA type 35 plus Canberra

on

109

10

TO 1V WTIME IN HOURS

26 30

Figure (39) : The half-life curve of 9 9 m T c

4.2.2 Determination of Radiocontamiiiants in Old ^ T e Generators :

Three Molybdenum-Technetium generators of the same total activity

(Amersham), one was 12 months old, the other 9 months old and the

third 6 months old were used for determination of the radiocontaminants99appearing with Mo. The gamma spectrum of these generators was

counted by using the multichannel analyser, type Pareke of KACST*

using a well type germanium detector. The results are shown in tables

(22, 23, 24). Although some of the data given in these tables are not

reasonable because of the very short half-life isotopes given in it, in

spite of the long cooling period, yet it indicates the persence of the

other long-lived fission products, 95Zr- 95Nb, 103Ru, 125Sb and 207Bi

showing the necessity to have good precautions in getting rid of these

types of genertor systems. Measuring these three generators again

using our MCA type 35 plus shows that they still contain some sort of

activity. The peaks of these activities appear on channels 19, 27, 41,

58, 157, and 190 indicating an energy of 63 KeV, 90 KeV, 136 KeV, 193

KeV, 523 KeV and 633 KeV respectively. In a trial to determine the

half-life of the 6 peaks analysis of composite decay curves was plotted

(Figures 40 - 45). Each decay curve is composed of two or more

components which requires very careful analysis, from this analysis, it

can be said that the main radioactivity is due to an isotope of half life

38.7 d. This isotope may be either Ru ( t 1 / 2 = 39.35 day, ,

497, 610 KeV) or 9 5 N b ( t l /2 = 3 5 d ) ^ d a u g h t e r P ™ ^ of 95Zr

= 65d). The second component shows a half life of approximately*fhese generators were kindly counted by Mr. Al-Medainy an engineer

in KACST.

SAMPLE•fission products absorption in aluminum column

M t : about 5 grams

DETECTOR SYSTEMORTEC Detec tor GMX20190, CFG-SV 301 ,MA:572, HV-PS-.459, Ana lysa to r : ADCAM 100 w i t h 91BAMCB and IBM A"

CALIBRATIONc a l i b r a t i o n measurements o-f eu-152 sourcecounted -for 1200 second

FIRST LIBRARY FILE FISSI0N1.LIB FBC

START 100 STOP 8000 SENS <7.) BO.O MULTIPLIER 7400.000

* * * * * * * * * * * * * * * * SUMMARY OF NUCLIDE3 IN SAMPLE * * * * * * * * * * * * * * * *

TIME OF COUNT PERCENTNUCLIDE ACTIVITY UNCERTAINTY

Bq/g COUNTING 2 S

AS-106 9.731E+02 1.1AR-41 1.525E-01 79.4 .BA-131 B.397E+01 2.731-214 3.142E+00 27.3ER-SO 1.11OE+02 7.5CE-144 7.040E+00 16.9IN-116M 2.156E-01 79.4NB-95 7.710E+00 4.4MD-141 2.363E+02 12.6NAT-RA 3.216E+00 26.6R'J-103 3. S04E+01 3.0RL!-105 2.700E+00 19.4SB-124 1.OOSE-01 74.1SB-125 1.S96E+00 39.4

* * * * * * * * * * * * * * * * * * * * * * * * * * SUMMARY * * * * * * * * * * * * * * * * * * * * * * * * * *TOTAL ACTIVITY: 1468.54

* * * * * * * * * * * * * * * * * * * * * DISPOSITION OF PEAKS * * * # * * * * * * * * * * * * * * * -

380.43 <§ SB-125 557.04 + RU-103 610.33 + RU-103665.45 e BI-214 1120.29 ? BI-214 1292.64 ? ND-141

1764.49 BI-214

Table (22) The radiocontaminants of 12 months old of Molybdenum-

Technetium generators counted by KACST.

nSr absorption in aluminum columnNo. 609/mon, wtsabout 5 grams 112

DETECTOR SYSTEM

5S

of eu-152

counted for 1200 second

FIRST LIBRARY FILE FISSICN2.LIBSTART 100 STOP B000 SENS (7.) 30.0 MULTIPLIER 7400.000

SUMMARY OF NUCLIDES IN SAMPLE ********************************

TIME CF COUNTNUCLIDE ACTIVITY

Bq/g -

1.B63E+02< 4.6E-011.305E+024.471E+00< 1.4E+012.502E+01< 7.2E-013.243E-K>1< B.9E*014.471E+004.973E+O1< 1.4E-i-0i< B.4E-013.470E+00< 1.3E+001.3B5E+00< B.5E-019.B3rE-011.458E+01< 5.SE-C1< 3.3E-01< i.4E+00< 1.OE+00< 2.4E+01

PERCENTUNCERTAINTYCOUNTINB 2 S

B.2

5.O54.7

14.B

4.4

54.76.B

53.5

70. B

79.79. 1

* * * * * * * * * * * * * * * * * * * * * * * * * * SUMMARY * * * * * * * * * * * * * * * * * * * * * * * * * *TOTAL ACTIVITY: 459.316

* * * * * * * * * * * * * * * * * * * * * DISPOSITION OF FEfiKS * * * * * * * * * * * * * * * * * * * * *

5">.2O S PA-230427 .39 * S3-125469 .37 @ RU-105696 .49 <§ CE-144

1293.54 ! IN-116M

60.11 « CE-144<43.75 @ PA-230557.04 @ RU-103717.34 @ AG-106N

21B5.70 ? CE-144

133.54 @ CE-144454.95 © PA-230610.33 + RU-103724.21 ! RU-105

99 99mTable (23) : The radiocontaminants of 9 months old of Mo - Tc generator

IfATCT

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10'

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2 . Composite decay curve

Shorter-lived component

20 300

TIME IN DAYS

Figure (kO) :• Composite decay curve of the peak at Channel 19

115

10'

8 •

6 .

k

Composite decay curve

Longer-VTved component

• Shorter-lived component

20 60 100 140 180

TIME IN DAYS

220 260 300

Figure (k^) : Composite decay curve of the peak at Channel 27

116

cr

si6

Composite decay curve

10

86

8

6

Longer-1iv»d component

Shorter-lived component

20 100 140 180

TIME IN DAYS

Figure Ct2) : Composite decay curve of the peak at Channel

117

Composite decay Curve

Shorter-lived component

20 60 100 1A0 180 220 260 300TIME IN DAYS

Figure C»3) : Composite decay curve of the peak at Channel 58

103

8 .

6 .

Composite decay curve

c'icr

Longer-Pi^ed component

I

Shorter-lived component

100 140 180 Z20 260 300TIME IN DAYS

20 60

Figure (kk) Composite decay curve of the , " :k at channel 157

119

10

Composite decay curve

Shorter-lived component

60 100 VkO 180 220 260 300TIME IN DAYS

Figure (̂ 5) : Composite decay curve of the peak at Channel 190

175 d which may be due to other long lived isotopes, again a case which

one must be very careful during working with these jcenerators.

4.2.3 Quality Control by Thin Layer Chromatography (TLC) and Paper

Chromatography :

To find out a method for determining the labelling yield by mTc,

thin layer chromatography as well as paper chromatography were

treated. Silica gel plastic sheet 2.5 cm x 20 cm of 0.2 mm thickness

with flou re scent indicator F™-. (Merk), celeluse plastic sheets 2.5 cm x

20 cm of 0.1 mm thickness without flourescent indicator (Merk), and

Whatman paper No. 1 (3.5 x 20 ), methanol and water (85:15, V/V) was

used as an eluent. 10 ul of each sample was chromatographed for 45

minutes after which the R- value was determined either by activity

counting in case of Tc or mTc labelled oil and !„ vapour in case

of unlabelled oil.

For counting, the chromatogram was devided into 1 cm sections then

cutting these parts and counting in the well type Nal (T£. ) gamma

detector.

The results are shown in tables (25, 26, 27). From these tables it

appears that paper chromatography gives a very good and clean

separation for 99mTc as 9 9 mTc04 and olive oil. Silica gel sheets give

two Rf values in case of olive oil, one having 0.78 value and is very

TABLE (25) : THE R f VALUES USING THE PLASTIC

SHEETS COATED WITH SILICA GEL

Sample Detect ion

01ive o i l

Oleic acid

1

0 (main peak)

0.78

04. - 0.8

Activi ty

I_ - vapor

I- - vapor

TABLE (26) : THE R f VALUES USING THE PLASTIC SHEETS

COATED WITH CELELUSE (0.1mm )

Sample

TcO"

01 ive ~>\ !

Oleic acid

R f

0.9

0

0.17-0.96

Detection

Activi ty

l 2 - vapor

l 2 - vapor

TABLE (27) THE Rf VALUES USING THE WHATMANN

PAPER 1

Sample

TcOJj

Olive o i l

Oleic acid

R f

0.78

0

Not regular

Detect ion

Activi ty

l_ - vapor

1- - vapor

122

small and may be attributed to degradation products in the oil while the

main peak has an R~ value of zero.

The R- value for mTc VII in paper chromatography was 0.78

which differs from that given in the literature i.e. 0.64 (96) and 0.6

(134) using Whatman paper 3 mm. The difference may be attributed to

the difference in the type of paper as well as the method of 99mTc

preparation. As labelling yield of olive oil with technetium as TcOT was

very low (section 4.2.4) it was found to be of value to try the labelling

using reduced mTc. Among the various reducing agents cited in the

literature (111, 112, 113) the most popular agent has continued to be

stannous ion. To study the effect of stannous ion Sn concentration

on the reduction of Tc, paper chromatographic technique was used.mTc (as eluted from the generator is mainly in the form mTcO~ ) in

diethyl ether as well as in acetone in the presence of different

concentrations of stannous ion was chromatographed. The results are

shown in Figures (46 - 55) and tables (28, 29). From the figures and

tables it appears that the R- "alue of mTc decreases as the

concentration of stannous ion increases meaning that the reduced

techniteum gives an R- of low value. Some of the activity is

homogenously distributed through the whole paper giving a percentage

of approximately 38 - 45% which may be in the colloidal Sn form. The

parts that have Rf >0.8 may be attributed to some sort of complex

having Tc in the oxidation state of VII since no higher state than

VII can be obtained and this shows a value of 2-15% in case of 20 mg

2600

Figure C»6) : "mTc in diethyl ether

PAPER CHROMATOGRAPHYAnalysis of 7*0—99m

s eDistance (Cm)

99m,

1600

Figure (i»7) : Tc in diethyl ether

PAPER CHROMATOGRAPHYAnalysis of Te—99m+2mg SnCl

a eDistance (Cm)

1600

Ftgure (kB)

PAPER CHROMATOGRAPHYAnalysis of Tc-99m+5mg SnCl in DEE

Distance (Cm)IN

Figure

1500

PAPER CHROMATOGRAPHYAnalysis of Tc—99m+10mg SnCl in DEE

3 eDistance (Cm)

Figure (50) :99m.Tc in diethyl ether

600

'400-

PAPER CHROMATOGRAPHYAnalysis of Tc-99m+20mg SnCl

a eDistance (Cm)

99m

2600

Figure (51) : Tc in Acetone

PAPER CHROMATOGRAPHYAnalysis of Tc—99m

2000

i1500

1000

600-

s eDistance (Crn)

vu

(uiw/bg) X11AI1DV

Figure (53)

1600

PAPER CHROMATOGRAPHYAnalysis of Tc—99m+ 5 mg SnCl in Aceton

3 eDistance (Crri\

Figure

400

PAPER CHROMATOGRAPHYAnalysis of Tc~99m+10mg SnCl in Aceton

3 aDistance (Cm)

1000

Figure (55)

PAPER CHROMATOGRAPHYAnalysis of Tc-99m+20mg SnCl in Aceton

3 6

Distance (Cm)

133

99mTABLE (28) : THE RVALUES FOR Tc UN DEE MEDUM)

MILKED AND REDUCED USING THE REDUCINGAGENT SnCl2 IN DIFFERENT QUANTITIES(2, 5, 10, AND 20 mg)

R fvalues

0

0.11

0.22

0.33

O . U

0.56

0.67

0.78

0.89

1

Milked

0

0

0

0

0.5

0.9

5-7

92.if

0.5

0

D i f f e r e n t

2 mg

0

0

0

0

0

2

95

3

0

0

Percentage of A c t M

Quantities of SnCl 9

5 mg

0

0

0

0

0

2

95

3

0

0

10 mg

15

0.5

0.5

0.5

0.5

0.5

80

0.5

0.5

0.5

i/ i ty

20 mg

U.8

3.8

3.8

3.8

3.8

3-8

3-8

3.8

3.8

15

13*

TABLE (29)99m

T ( I N ACETONE MEDIUM)

MILKED AND REDUCED USING THE REDUCING AGENT

: THE R f VALUES OF

Sn C l 2 IN DIFFERENT QUANTITIES ( 2 , 5 , ± 0 , AND

20 mg )

R fValues

0

0.11

0.22

0.33

O . U

0.56

0.67

0.78

0.89

1

I

P E R C E N T A G E OF A C T I V I T Y

M I L K E D

0

0

0

0

0 .5

7

11 .5

7 7 . 9

2 . 8

0

D I F F E R E N T Q U A N T I T I E S OF SnCl

2 mg

0

0

0

1

1 . 7

i * .1

8 1 . 8

9 . 6

1

0

5 mg

0

0

0

0

21

* . 9

8 3 . 6

8 .2

0 . 7

0

10 mg

7

10

7 -6

8

6 - 7

7

2 7 . 3

1 2 . 1 3

7 . 1

6 . 9

20 mg .

(,k

13

3 . 5

3

k.G

3-9

2

2

2 . 5

0

135

Jin in view of what is stated in the literature the complex Sn

"CcHg may be that what have the Rf >0.8.

Despite the fact that the chemistry of the element (Tc) is poorly

developed in comparison to its immediate neighbours Mo, Mn> Ru, and

Re, there is no shortage of review articles dealing with various -aspects

oJ" its chemistry (120). From what is known, it is to be expected that

its chemistry will be proved to be among the most diverse of the

transition elements certainly revealing that of its second row neighbours

Mo and Ru. Compounds have already been characterized in all

oxidation states from (-l)d8, e.g. [ Tc(COj5fto VII d°,e.g. TcO" (121)

and TcHg (122) in which the elements displays coordination numbers

which vary from 4 to 9. The most exciting recent development and

perhaps the most relevant to nuclear medicine is that a number of the

lower valent complexes can be synthesized in high yields in aqueous

media at both the carrier and no-carrier-added concentrations.

The octahedral d , hexachlorometallates inflamed by heating TcO"

salt in the corresponding halo acid HX. (X is a halogen in this case Cl)

TcO" + 3H3O+ + 9X"

in presence of concentrated acid prevents hydrolysis to TcO™ at low

temperature.

136

+ 6H O+ + 6 x ' (TcOX^)" + 9H 0 + X

However, both elec trophoresis and adsorption spectrum studied by

Ianovici et al (123) shows that about 15% of the Tc Cl^2 hydrolysed to

other species.

The hydrolysed Tc Cl"2 appears as cationic, uncharged and anionic

species TcCl-(Ho0)]~ (124)

The anionic species was reported by Kawashima (124) as

[TcClj.(H2O)] . The unchanged species is more likely to be a mixture of

hydrated TcO 'and [ TcCl4(H2O)2](125). Concerning the nature of the

cation it was expected that its spectrum would resemble that reported

for [TcCl3(H2O)3] + (126, 127).

The neutral species (formed by hydrolysis and'or isometric

transition) can be easily oxidized to TcO^ by air (128, 129) but the

proportion oxidized decreases rapidly as the chemical concentration of

technetium increases. Possibly the aerial oxidation only proceeds

rapidly in true solution and becomes negligible when a colloidal

TcOo x HOO phase forms (123.). It appears that what we have in thisii it

work is a mixture of different cationic, anionic uncharged and colloidal

species and that colloidal and unchanged species increase with the

increase of Sn Cl™ concentrations. Of course intensive concentration of

this part need more work which is out of the scope of this thesis.

137

In addition to the last indicated complexes we may give the

following oxidation reduction icn equations.

Tc O ' + Sn+2 + 2H+ TcO~ + Sn+4 + H2O (130)

from Tc VII to Tc V

2Tc OT + 3Sn+2 + 8H+ 2Tc O9 + 3Sn+4 + 4HOO (128)4 L I

to reduce Tc VII to Tc IV

T c 0 4 + 2Sn+2 + 4H+ TcO2 + 2 S n + 4 + 2 H 2°

to reduce Tc VII to Tc III

2TcO~ + 5Sn+2 +16 H+ 2Tc?2 + 5Sn+4 + 8 H2O (132)

to reduce Tc VII to Tc II+2indicating that increase of concentration of Sn leads ,the reaction to

proceed more to reduction and complicates the problem. This indicates+2that the concentration of Sn is critical (133).

138

4.2.4 Labelling of Olive Oil by 9 9 mTc :

In a 5 ml round bottom flask 2 ml diethyl ether or acetone were

added, followed by 1 mCi of"mTcO4 (100 u 1) then a 30 yl of olive oil

was added. The whole solution was stirred by magnetic stirrer at room

temperature, and samples (10 yl) were withdrawn at different periods of

time and analyzed by paper chromatography. The results are given in

table (30) showing a percent yield of 1.8% to assure that mTc in the

VII state is responsible for the low labelling yield, the labelling

experiment was repeated by using Tc to which bromine water was

added. The results (precent yield 0.5%) show no change in labelling

yield indicating the urgent need for reducing mTc in order to get

labelling.

4.2.5 Labelling of Olive Oil by reduced 9 9 m Tc:

A. In Diethyl ether (DEE) medium :

In a 5 ml round bottom flask 2 ml of acidified diethyl ether of

pH( l -2 ) , prepared by shaking ljO ml 6N HC1 with 10 ml DEE and taking

the DEE layer, was added. Then 1 mCi of TcO4 (100 y 1) was

added, followed by the reducing agent SnCl2 .2H2O, (2, 5, 10, or 20

mg). The flask was shaken vigorously for 2 - 3 minutes after which 30

1 of olive oil were added. The whole solution was stirred by magnetic

st i rrer at room temperature, and samples (10Pi) were withdrawn at

different periods of time and analyzed by paper chromatography. The

TABLE (30) : LABELLING YIELD OF OLIVE OIL BY99m

(IN DEE AND ACETONE

MEDIUM

139

Time in

minutes

10

30

60

90

Acetone

1

1

1

1

8

.2

.2

Label 1i ng

medium

Y i e l d

DEE

1 .

1

1

0 .

Percentage

medi urn

5

8

results are given in Figure (56) showing that more than 50% labelling

yield was attained within the first 10 minutes in case of 20 mg Sn .

B. In Acetone Medium :

In a 5 ml round bottom flask we add 2 ml of acidified acetone of pH

1-2 prepared by addition of 1 ml 6NHC1 to 9 ml acetone followed by 1

mCi of 9 9 mTc04 (100 Ul) then we add the reducing agent SnCl2.2H2O (2

mg or 5 mg, 10 mg or 20 mg). The flask was shaken vigoursly for 2 -

3 minutes after which 30PI of olive oil were added. The whole solution

was stirred by magnetic stirrer at room temperature, and samples were

withdrawn at different periods of time and analyzed by paper

chromatography. The results are shown in figure (57). The curve

shows that labelling took place within the first 10 minutes and that

labelling increased with the increase of reduced species resulting from+2increase concentration of Sn ion, which is in good agreement with

work done on labelling of the phosphonates and other radio-

pharmaceuticals with 99mTc (133).

Figure (56)

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Time (min)

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