Design and Testing of Boost Converter Under the Guidance of
Transcript of Design and Testing of Boost Converter Under the Guidance of
JSS MahavidyapeethaSri Jayachamarajendra College of Engineering, Mysore 570 006
An Autonomous Institution Affiliated toVisvesvaraya Technological University (VTU), Belgaum
Design and Testing of Boost Converter
Thesis submitted in partial fulfillment of the curriculum prescribed for theaward of the degree of Bachelor of Engineering in Electrical and
Electronics Engineering by
4JC08EE047 Sathish Kumar D4JC09EE400 Basavaraju C4JC09EE406 Nagendra Prasad M N
Under the Guidance of
M.H.SidramAssociate Professor
Department of E&EE, SJCE, Mysore
Department of Electrical & Electronics Engineering
June, 2012
JSS MahavidyapeethaSri Jayachamarajendra College of Engineering, Mysore 570 006
An Autonomous Institution Affiliated toVisvesvaraya Technological University (VTU), Belgaum
CertificateThis is to certify that the work entitled “Design and Testing of Boost Converter” is abonafide work carried out by Sathish Kumar.D, Basavaraju.C, Nagendra Prasad.M.Nin partial fulfillment of the award of the degree of Bachelor of Engineering in Electrical andElectronics Engineering of Visvesvaraya Technological University, Belgaum, during theyear 2012. It is certified that all corrections / suggestions indicated during CIE have beenincorporated in the report. The project report has been approved as it satisfies the academicrequirements in respect of the project work prescribed for the Bachelor of EngineeringDegree.
GuideM.H.Sidram
Associate ProfessorDepartment of E&EESJCE, Mysore 570 006
Head of the DepartmentR.S.Ananda Murthy
Associate Professor and HeadDepartment of E&EESJCE, Mysore 570 006
Date :Place : Mysore
Examiners : 1._____________________________
2._____________________________
3._____________________________
Abstract
The power electronics is fast developing technology with wide applications in the industrial and
power sectors. This motivated us to chose the power electronics field for our project.
This project deals with the designing of power electronics DC-DC boost converter. The objec-
tive of the project serves its purpose mainly in Solar PV stand-alone installations. A MOSFET based
boost converter was designed to run in Continuous Conduction Mode (CCM) with the achievement
of 68% efficiency.
In this project report we have presented the basics of boost converter design, selection criteria
of various components employed and the inductor design procedure.
i
Acknowledgements
We are immensely grateful to Mr.R.S.Ananda Murthy, Head of the Department of Electrical and
Electronics Engineering, SJCE Mysore, for giving us an opportunity to carryout our project work.
Also we would like to thank him for his support and encouragement throughout our project.
We take this opportunity to express our deep sense of gratitude and indebtedness to our project
guide Mr. M.H.Sidram, Associate Proffesor, Department of Electrical and Electronics Engineering,
SJCE Mysore, for his inspiring guidance, constructive criticism and valuable suggestion throughout
this project work.
Also we are very thankful to Dr.B.G.Sangameshwara, Principal of SJCE, Mysore, for providing
the necessary infrastructure and support.
We would also like to thank all teaching and non-teaching staff of our department who directly
or indirectly contributed in the accomplishment of this task.
Our sincere thanks to all our friends who have patiently extended all sorts of help for accom-
plishing this undertaking.
ii
Contents
Contents iii
1 Introduction to DC-DC Converters 11.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
1.2 Types of DC-DC converter . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
The functions of DC-DC converters are: . . . . . . . . . . . . . . . . . . . . . . . 2
Applications . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
2 Basics of Boost Converter 42.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
2.2 Operation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5
Continuons Conduction Mode . . . . . . . . . . . . . . . . . . . . . . . . . . . . 6
Discontinuons Conduction Mode . . . . . . . . . . . . . . . . . . . . . . . . . . . 8
2.3 The important features of Boost converter . . . . . . . . . . . . . . . . . . . . . . 10
3 Components Selection Criteria 113.1 Power Stage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11
Selection of Semiconductor Device . . . . . . . . . . . . . . . . . . . . . . . . . 11
Selection of Inductor . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 13
Selection of Diode . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14
Selection of Capacitor . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14
3.2 PWM Control and Driver Circuit . . . . . . . . . . . . . . . . . . . . . . . . . . . 15
4 Design of Boost Converter 164.1 Block Diagram . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 16
4.2 Theoretical Calculation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17
4.3 Inductor Design . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19
4.4 Main Circuit Diagram . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20
5 Result and Conclusion 21
iii
Contents iv
5.1 Triggering pulses as viewed on CRO . . . . . . . . . . . . . . . . . . . . . . . 21
5.2 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23
Future Advancement . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23
Appendix-1 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 24
Appendix-2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26
Bibliography 59
Chapter 1
Introduction to DC-DC Converters
1.1 Introduction
In many industrial applications, it is required to convert a fixed voltage DC source into a variable
voltage DC source. A DC-DC converter can be considered as DC equivalent to an AC transformer
with a continuously variable turns ratio. Like a transformer, DC-DC converter can be used to step
up or step down a DC voltage source.
Modern electonic systems require high-quality, small, lightweight, reliable, and efficient power
supplies. Linear power regulators, whose principle of operation is based on a voltage or current
divider are inefficient. This is because they are limited to output voltages smaller than the input
voltage, and also their power density is low because they require low frequency (50 or 60Hz) line
transformers and filters. Linear regulators can, howerver, provide a very high quality output volt-
age. Their main area of application is at low power levels. Electronic devices in linear regulators
operate in their Active (linear) modes, but at higher power levels switching regulators are used.
Switching regulators use power electronic semiconductor switches in ON and OFF states. Because
there is a small power loss in those states (low voltage across a switch in the ON state, zero cur-
rent through a switch in the OFF state), switching regulators can achieve high energy conversion
efficiencies. Modern power electronic switches can operate at high freuencies. The higher the
operating frequency, the smaller and lighter the transformers, filter inductors, and capacitors. In
addition, the dynamic characteristics of converters improve with increasing operating frequencies.
The bandwidth of a control loop is usually determined by the corner frequency of the output filter.
Therefore, High operating frequencies allow for achieving faster dynamic response to rapid
changes in the load current and/or the input voltage. High frequency electronic power processors
are used in DC-DC power conversion.
1
Chapter 1. Introduction to DC-DC Converters 2
1.2 Types of DC-DC converter
The DC-DC converters can be divided into two main types:
(1) Hard-switching pulse width modulated (PWM) converters
(2) Resonant and soft swtching converters.
Advantages of PWM converters include low component count, high efficiency, constant fre-
quency operation, relatively simple control and commercial availability of integrated circuit con-
trollers, and ability to achieve high conversion ratios for both step-down and step-up application. A
disadvantage of PWM regulator voltage and current waveforms cause turn-on and turn-off losses in
semiconductor devices, which limit practical operating frequencies to hundreds of kHz. Rectangu-
lar waveforms also inherently generate Electro Magnetic Interference (EMI).
• Buck Converter
• Boost Converter
• Buck-Boost Converter
For our project we are to make a boost converter, also known as a step-up converter. We are
to design our own circuit layout on PCB and design our own inductor. Our boost converter is to
have an input voltage of 20V to 24V and an output of 110V. We are to increase or decrease the load
resistance in order to achieve a continuous conduction mode at a 220 Watts output. The switching
frequency of the switch should be 60 kHz and the output voltage ripple should be 1%. The major
components that we have used in our circuit are IRF840 MOSFET , the BYQ28E Fast recovery
diode, and an output capacitor of 33 uF. For the PWM controller we are to use the SG3524 with an
inbuilt gate driving capability. Together with all our components and our own made circuit board
we were able to achieve our goal of an output of 110V.
The functions of DC-DC converters are:
• To Step up a Low DC input voltage.
• To regulate the DC output voltage against load and line variations.
• To reduce the ac voltage ripple on the dc output voltage below the required level.
• To provide isolation between the input source and the load (isolation is not always required)
• To protect the supplied system and the input source from electromagnetic interference (EMI).
Chapter 1. Introduction to DC-DC Converters 3
Applications
1. DC-DC converters are used in battery powered electronic devices such as MP3 players, Lap-
tops etc
2. Switched Mode Power Supply (SMPS).
3. Adjustable speed drives.
4. Hybrid Electric automobiles.
5. They are widely used in Traction motor control.
6. Also used in trolley cars, marine hoists, forklift trucks and mine haulers.
Chapter 2
Basics of Boost Converter
2.1 Introduction
Boost converter is a type of DC-DC converters which steps up the input voltage to a higher value.
The DC-DC converters are widely used in regulated switch mode DC power supplies. The input of
these converters is an unregulated DC voltage, which is obtained by PV array and therefore it will
be fluctuated due to changes in radiation and temperature. In these converters the average DC output
voltage must be controlled to be equated to the desired value although the input voltage is changing.
From the energy point of view, output voltage regulation in the DC-DC converter is achieved by
constantly adjusting the amount of energy absorbed from the source and that injected into the load,
which is inturn controlled by the relative durations of the absorption and injection intervals. These
two basic processes of energy absorption and injection constitute a switching cycle. Intuitively
speaking, if the energy storage capacity of the converter is too small or the switching period is
relatively too long,then the converter would have transmitted all the stored energy to the load before
the next cycle begins. This introduces an idling period immediately following the injection interval,
during which the converter is not performing any specific task.
An ideal boost converter is lossless in terms of energy, so the input and output power are equal.
In practice, there will be losses in the switch and passive elements, but efficiencies better than 90%
are still possible through careful selection of system components and operating parameters such as
the switch frequency.
The DC-DC boost converter only needs four external components: Inductor, Semiconductor
switch, Diode and output capacitor. The converter can therefore operate in the two different modes
depending on its energy storage capacity and the relative length of the switching period. These two
operating modes are known as the discontinuous conduction mode, DCM, and continuous conduc-
tion mode, CCM, corresponding to the cases with and without an idling interval respectively.
Fig 1 shows the circuit diagram of Boost converter. The Boost converter has two modes, a
continuous conduction mode, CCM for efficient power conversion and Discontinuous conduction
4
Chapter 2. Basics of Boost Converter 5
mode, DCM for low power or stand-by operation.
Fig.1 Basic circuit diagram
Where Vg= Input DC voltage
L = Inductor
C = Storage capacitor
v = Output DC voltage
2.2 Operation
The Boost converter has two modes,
• Continuons Conduction Mode, (CCM) and
• Discontinuons Conduction Mode (DCM).
Fig 2. Circuit Schematic of Step-up DC/DC Converter
The working of boost converter can be explained in two phases based on the switch (MOSFET)
operation. Depending upon the output required, the duty cycle of the triggering pulse to the switch
has to be provided. All the calculation details are provided in chapter 3.
Chapter 2. Basics of Boost Converter 6
Continuons Conduction Mode
Mode 1 (0 < t ≤ ton)
Mode 1 begins when MOSFET is switched on at t =0 and terminates at t = ton. The equivalent
circuit for the mode 1 is shown in Fig.3(a) The inductor current iL(t) greater than zero and ramp up
linearly. The inductor voltage is Vi.
Mode 2 (ton < t ≤ Ts)
Mode 2 begins when MOSFET is switched off at t = ton and terminates at t = Ts. The equivalent
circuit for the mode 2 is shown in Fig.3(b). The inductor current decrease until the MOSFET is
turned on again during the next cycle. The voltage across the inductor in this period is Vi−V0.
Since in steady state time integral of the inductor voltage over one time period must be zero.
Viton +(Vi−V0) to f f = 0
Where;
Vi : Input voltage, volts.
V0 : Average output voltage,volts
ton : On time of the MOSFET, s
to f f : Off time of the MOSFET, s
Dividing both sides by Ts and rearranging the terms yield
V0
Vi=
Ts
to f f=
11−D
Where;
Ts: Switching period, s.
D : Duty cycle.
Chapter 2. Basics of Boost Converter 7
Fig 3. Equivalent Circuit for boost Converter in CCM
(a) Mode 1 (0 < t ≤ ton)
(b) Mode 2 (ton < t ≤ Ts)
Thus, V0 is inversely proportional to (1-D). It is obvious that the duty cycle ’D’, can not be equal
to 1 otherwise there would be no energy transfer to the output. Assuming a lossless circuit,Pi =
Po,then
IiVi = IoVo
and,
Io
Ii= 1−D
Where;
Io: Average output current, Amp.
Ii: Average input current, Amp.
Chapter 2. Basics of Boost Converter 8
Discontinuons Conduction Mode
If the current following through the inductor falls to zero before the next turn-on of the switching
MOSFET, then the boost converter is said to be operating in the discontinuous conduction mode. If
we equate the integral of the inductor voltage as shown in Fig.4 over one time period to zero,
ViDTs +(Vi−V0)D1Ts = 0
Then,
V0
Vi=
D1 +DD1
and
I0
Ii=
D1
D1 +D
(since Pi = Po)
Fig.4: Equivalent Circuit for boost Converter in DCM
(a) Mode 1 (0 < t ≤ ton)
(b) Mode 2 (ton < t ≤ (D+D1)T s
(c) Mode 3 (D+D1)Ts < t ≤ Ts
From Fig.4(c), the average input current, which is equal to the inductor current, is
Ii =Vi
2LbDTs (D+D1)
Chapter 2. Basics of Boost Converter 9
I0 =
(ViTs
2Lb
)DD1
In practice, since Vo is held constant and D varies in response to variation in Vi, it is more useful
to obtain the required duty cycle ’D’, as a function of load current for various values of Vo/Vi.
Now,
D =
[427
V0
Vi
(V0
Vi−1
)I0
I0,aver,max
]0.5
Where;
Io,aver,max : The maximum average output current at the edge of continuous conduction and can be
found by the following equation.
I0,aver =TsV0
2LbD(1−D)2
The average output current has its maximum at D=1/3.
I0,aver,max =2
27TsV0
L
The critical inductance, Lc, is defined as the inductance at the boundary edge between continu-
ous and discontinuous modes and is defined as:
Lc =RD(1−D)
2Fs
where;
R : Equivalent load resistance,Ω
Fs : Switching frequency, Hz
The switching frequency has been chosen arbitrarily to minimize the size of the boost inductor
Chapter 2. Basics of Boost Converter 10
and limit the loss of the semiconductor device. At higher frequencies the switching losses in the
MOSFET increases, and therefore reduces the overall efficiency of the circuit. At lower frequencies
the required output capacitance and boost inductor size increases, and the volumetric efficiency of
the supply degrades.
2.3 The important features of Boost converter
1. The gain is more than unity.
2. The gain is independent of switching frequency as long as Ts RC. However this design
inequality is a function of the load.
3. The output voltage ripple percentage is dependent on the load on the converter.
4. The parasitic resistances in the converter degrades the gain of converter.
5. The ideal efficiency is unity.
Chapter 3
Components Selection Criteria
3.1 Power Stage
As discussed in the previous chapter, the power stage can operate in continuous or discontinuous
inductor current mode. In continuous inductor current mode (CCM), current flows continuously in
the inductor during the entire switching cycle in steady-state operation. The current never reaches
zero. In discontinuous inductor current mode (DCM), inductor current is zero for a portion of the
switching cycle. It starts at zero, reaches a peak value, and returns to zero during each switching
cycle.
The main components of the power stage are namely inductor, semiconductor switching device,
Diode and capacitor. The selection procedure for these components is as follows,
Selection of Semiconductor Device
The main switching element has been chosen to handle the worst case current and voltage stresses.
The maximum voltage stress on the switching device occurs when the PV/RPS output voltage is
maximized, so:
Vmax,stress =Vin,max
Vin,max : is the maximum input voltage from PV array or RPS, Volt.
The maximum current stress occurs when system power is predominately provided by the PV.
Therefore, the peak current is
Ipeak = Iout put + Iripple
11
Chapter 3. Components Selection Criteria 12
Ipeak =Pin,max
Vin+4Pin,max
Vin
Where;
Pin,max : Maximum input to boost converter.
4: Percentage of ripple current to load output current.
MOSFET: The MOSFET, however, is a device that is voltage controlled and not current con-
trolled. MOSFETs have a positive temperature coefficient, stopping thermal runaway. The ON-
state-resistance has no theoretical limit, hence ON-state losses can be far lower. The MOSFET also
has a body-drain diode, which is particularly useful in dealing with limited freewheeling currents.
All these advantages and the comparative elimination of the current tail soon meant that the
MOSFET became the device of choice for power switch designs. Then in 1980’s the IGBT came
along .
IGBT: The IGBT has the output switching and conduction characteristics of a bipolar transistor
but is voltage controlled like a MOSFET. In general, this means it has the advantages of high-current
handling capability of a bipolar with the case of a control of a MOSFET. However, the IGBT still
has the disadvantages of comparatively large current tail and no body drain diode.
Early versions of the IGBT are also prone to latch up, but nowadays, pretty well eliminated.
Another potential problem with some IGBT types is the negative temperature coefficient, which
could lead to thermal runaway and makes the paralleling of devices hard to effectively achieve.
This problem is now being adressed in the latest generations of IGBTs that are based on “non-
punch through” (NPT) technology. This technology has the same basic IGBT structure but is based
on bulk-diffused silicon, rather than the epitaxial material that both IGBTs and MOSFETs have
been historically used.
It is interesting to note that an IGBT does not exhibit a BJT-like second breakdown failure.
Since, in an IGBT most of the collector current flows through the drive MOSFET with positive
temperature coefficient, the effective temperature coefficient of VCE in an IGBT is slightly positive.
This helps to prevent the second breakdown failure of the device and also facilitates paralleling of
IGBTs.
Choice between IGBTs and MOSFETs is very application-specific and cost, size, speed, switch-
ing loss and thermal requirements should all be considered. Hence the MOSFET IRF840 is chosen
for switching purpose.
Chapter 3. Components Selection Criteria 13
Selection of Inductor
Eventhough inductors and transformers are both magnetic components, there is a very important
difference in their functioning and design aspect. In a transformer, the core flux (or the flux density)
is decided by the magnetizing current. The load current virtually has no say in deciding the core flux
(the flux due to the load current is nullified by the counter flux produced by the primary component
of the load current) where as in an inductor, the core flux is decided by the load current. Thus
if the load current increases, there is a possibility that the core may saturate and inductance will
come down. So the primary consideration in inductor is that one has to know the maximum load
current and have the core which does not saturate at this current. This can lead to huge core size
if the current to be handled is high. The core size can be reduced considerably by introducing an
appropriate air gap in the magnetic circuit, with this the coil can carry considerably larger current
without saturating the core.
In switching regulator applications inductor is used as an energy storage device, when the semi-
conductor switch is ON the current in the inductor ramps up and energy is stored. When the switch
turns OFF this energy is released into the load, the amount of energy stored is given by,
Energy = 0.5(LI2
)joules
where L is the inductance in Henrys
and I is the peak value of the inductor current.
Inductor is the energy storage element in the boost converter circuit. Large inductance values
tend to increase the start-up time slightly while small inductance values allow the coil current to
ramp up to higher levels before the switch turns OFF. Inductors with a ferrite core or equivalent
are recommended. It should be ensured that the inductor’s saturation current rating for highest ef-
ficiency is to be used a coil with low DC resistance. Boost inductance is selected based on the
maximum allowed ripple current at minimum duty cycle ’D’ at maximum input voltage, Vin. Given
that switching frequency, Fs, the boost inductor value may be optimally determined to set the con-
verter operating mode in the required load and line range. The critical inductance is defined as the
inductance at the boundary edge between continuous and discontinuous modes. So the value of the
inductor assuming the inductor ripple current4I = 2Io is given by the formulae.
Lmin = (1−D)DR/2Fs in Henry.
where ,
Fs= Switching frequency in Hz
D = Duty cycle
R = The equivalent load, Ω
Keeping this value as reference one can decide what should be the value of inductor by per-
Chapter 3. Components Selection Criteria 14
forming simulation to reduce the starting current. For our project EE type ferrite core inductor is
used with 13 SWG thickness of the wounded copper along with the bobbin.
One thing to note about the Boost converter topology is that the inductor current does not con-
tinuously flow to the load. During the switch ON period the inductor current flows to ground and
the load current is supplied from the capacitor. This means that the output capacitor must have suf-
ficient energy storage capability and ripple current rating inorder to supply the load current during
this period.
Selection of Diode
The Boost diode reverse voltage is limited to the output voltage. The diode conducts when the power
switch is in the OFF state and provides a current path for the inductor to the output. Similar to the
IGBTs the worst-case peak current through the diode occurs at low line input voltage and maximum
load. Other important considerations in selecting the diode besides its ability to block the required
OFF-state voltage stress and have sufficient peak and average current handling capability, is fast
switching characteristics, low reverse recovery, and low forward voltage drop.
Since The switching frequency is 60kHz, the diode should be fast enough to operate. Hence
fast recovery diode, BYQ28E which is rated for 500V , 10A is chosen.
Selection of Capacitor
The primary criterion for selecting the output filter capacitor is its capacitance and equivalent series
resistance, ESR. Since the capacitor’s ESR affects efficiency, low-ESR capacitors will be used for
best performance. For reducing ESR is also possible to connect few capacitors in parallel. The
output filter capacitors are chosen to meet an output voltage ripple specifications, as well as its
ability to handle the required ripple current stress.
As mentioned earlier the capacitor should be able to store the complete energy when the switch
is OFF. So the minimum value of the capacitance assuming the capacitor ripple voltage4Vc = 2Vo
is given by the formulae,
Cmin = D/2FsR in Farads
where,
Fs = Switching frequency in Hz
D = Duty cycle
R = Equivalent load, Ω.
Chapter 3. Components Selection Criteria 15
3.2 PWM Control and Driver Circuit
The stability of the boost converter will depend on the type of control loop. The main purpose of
the driver circuit is to enhance the switching voltage for the MOSFET or any other switching device
and also we have to isolate the power circuit from the control circuit. Because the power circuit
current must not enter into the control/switching circuit. In our project we have used the PWM IC
SG3524 ( TEXAS Instruments make ) with a gate driving capability.
Fig 5.Pin Description of SG3524
Chapter 4
Design of Boost Converter
4.1 Block Diagram
The above fig shows the block diagram which includes,
1. Power Supply : 24V, 10A DC source as per our requirement
2. Boost converter : This block takes an input DC voltage at low level and gives out a Boosted
voltage, in this case it steps up 24 Volts DC to 110 Volts DC.
3. PWM Control : This gives the necessary gate pulses with required duty cycle for turning
ON the MOSFET
16
Chapter 4. Design of Boost Converter 17
4.2 Theoretical Calculation
CURRENT RIPPLE FACTOR (CRF):
By taking the current ripple factor of the inductor to be 40%.
i.e4II
= 40%
VOLTAGE RIPPLE FACTOR (VRF):
i.e4V0
V0= 1%
SWITCHING FREQUENCY (Fs):
Fs =1.3
Rt Ct=
1.32.2k ∗0.01µ
Fs = 60kHz
GIVEN DATA:
• Input voltage, Vg=24V
• Output voltage, Vo=110V
• Output load current, Io=2A
Step 1 : Calculation of Duty cycle (D):
V0
Vi=
11−D
11−D
=11024
D = 0.78
Chapter 4. Design of Boost Converter 18
With 110 volts 2 Amps output, This represent a load of 220W.
Assuming Efficiency to be 90% ( the effiency will be less than the assumed value for Practical
case).
Input power =2200.9
= 244W
With a 24 volts input, this represents average input current of 24424 = 10.16Amps
The optimal Ripple current of the inductor is 40% of the output current. This is a good thumb
rule for most DC - DC Converters and represents a trade off between small inductor size and low
switching losses.
Our inductor current is 10.16 Amps, so for 40% ripple the peak current needs to be (10.16 ∗1.2) = 12.2A. Our minimum inductor current needs to be (10.16∗0.8) = 8.13A.
This gives a change in current4I = 4A.
A switching frequency of 60 kHz has a period of,
T =1Fs
=1
60k= 16.6µs
So the MOSFET switches ON for tON = (0.78∗T ) = 13µs.
We have calculted that our4I needs to change by 4 A, so our change in current with time is,
dIdt
=4
13µ= 0.37∗106
VL = LdIdt
When MOSFET is turned ON Vi =VL = 24V
Therefore the value of inductance is given by
L =Vi/
(dIdt
)=
240.37∗106 = 65 µH
Now, if too much current flows in the inductor, the ferrite core that is wound may saturate with
the effect, that its inductance rapidly decreases. From the equation for Inductor value above, if the
inductance decreases the change in current with time increases, worsening the effect of over current
so we must ensure that the inductor we choose is rated to handle the current. Thus the saturation
rating of the inductor needs to be in excess of the peak current of 12.2 Amps. Therefore a saturation
rating of 13 A should suffice our purpose.
Chapter 4. Design of Boost Converter 19
4.3 Inductor Design
E = 0.5LI2 = 0.5∗65µ ∗10.162 = 3.35∗10−3 Joules
Assuming Bm = 0.2Tesla, J = 3A/mm2, Kc = 1, Kw = 0.6
Ap = Aw ∗Ac =2E
Kw Kc J Bm=
6.7∗10−3
36∗104 = 1.86∗10−8 m4
Where,
Ap= Area Product, m4
Aw= Window Area, m2
Ac= Core Area, m2
Kw= Window space factor
Kc= Crest Factor
J = Current Density
Bm= Maximum flux density
With this Calculated Area Product we can select the type of core required, refering to Appendix
- 1
So we have chosen EE 42/21/9
For the core selected,the values for Ap, Aw, Ac are obtained from Appendix-1 and are as follows,
Ap = 2.739∗104 mm4
Aw = 2.56∗102 mm2
Ac = 1.07∗102 mm2
N =LIm
Ac Bm= 32Turns
A =IJ=
10.163
= 3.38mm2
With this calculated Area of conductor (A) we get the conductor size of 13 SWG (Refer
Appendix-2)
The current through the capacitor is given by,
Ic =CdVdt
Assuming4v to be 1% of the output voltage4v = 1.1V
Chapter 4. Design of Boost Converter 20
For CCM Ic = Io, therefore the value of capacitor is given by,
C = Io/dVdt
= 2/(
1.113µ
)= 23.6µF
So we have chosen the value of capacitor to be 33µF .
4.4 Main Circuit Diagram
Chapter 5
Result and Conclusion
5.1 Triggering pulses as viewed on CRO
Vin in volts Vo in volts Duty cycle5 23 78%
10 46 78%
15 69 78%
20 90 78%
24 110 78%
21
Chapter 5. Result and Conclusion 22
The Results are valid when 4VoVo
=4V = DTsRC 1
In other words, the switching period (Ts) must be very much less than the natural period
(t0 = RC) of the converter.
Efficiency = Pout,wattsPin,watts
= 110∗0.324∗2 = 68%
Chapter 5. Result and Conclusion 23
5.2 Conclusion
With the analysis completed and the board fully designed and built, we found that our group suc-
cessfully designed a boost converter. A low input voltage (24 V) was applied and a high voltage
(110 V) was obtained according to the specifications that were given to us. As a group, we designed
a functioning PCB with only minor errors. Considering that we had no prior design experience, the
board’s minor errors were typical and could easily be corrected on another design. The boost con-
verter ran with an efficiency of over 60% in all data tests. With this knowledge of power electronics
and design, we feel that, as a group, we are better prepared for the future as engineers.
The Boost converter that we have designed can be loaded upto 2 Amps.With the inductor de-
signed for still higher peak current rating the loading capability of our converter can be increased
upto 4 Amps.
Future Advancement
• By incorporating the soft-start technique and by upgrading the rating of the devices we can
use the designed Boost Converter to drive DC Motors.
• By employing an inverter at the output stage of the Boost converter we can use it for Domestic
lighting.
• It can also be used to charge a Battery by employing Charge Controller.
Chapter 5. Result and Conclusion 24
Appendix-1
Cores
without air
gap
Mean
length per
turn in
mm
Mean
magnetic
length in
mm
Core
cross
section
area Ac ∗100mm2
Window
area Aw ∗100mm2
Area
product
Ap ∗104 mm4
Effective
relative
permia-
bility
µr±25%
AL
nH/turns2
±25%
POTCORES - CEL HP3C grade,(*Philip 3B7 grade)
P 18/11 35.6 26 0.43 0.266 0.114 1480 3122
P 26/16 52 37.5 0.94 0.53 0.498 1670 5247
P 30/19 60 45.2 1.36 0.747 1.016 1760 6703
P 36/22 73 53.2 2.01 1.01 2.010 2030 9500
P 42/29 86 68.6 2.64 1.81 4.778 2120 10250
P 66/56 130 123 7.15 5.18 37.03
EE - CORES - CELL HP3C grade
E 20/10/5 38 42.8 0.31 0.478 0.149 1770 1624
E 25/09/6 51.2 48.8 0.40 0.78 0.312 1840 1895
E 25/13/7 52 57.5 0.55 0.87 0.478 1900 2285
E 30/15/7 56 66.9 0.597 1.19 0.71
E36/18/11 70.6 78.0 1.31 1.41 1.847 2000 4200
E 42/21/9 77.6 108.5 1.07 2.56 2.739 2100 2613
E 42/21/15 93 97.2 1.82 2.56 4.659 2030 4778
E 42/21/20 99 98.0 2.35 2.56 6.016 2058 6231
E 65/32/13 150 146.3 2.66 5.37 14.284 2115 4833
UU - CORES
UU 15 44 48 0.32 0.59 1.90 1100
UU 21 55 68 0.55 1.01 0.555 4.25
UU 23 64 74 0.61 1.36 0.823 1425
UU 60 183 184 1.96 11.65 22.83 1900
UU 100 29.3 308 6.45 29.14 187.95 3325
Chapter 5. Result and Conclusion 25
TOROIDS - CELL HP3C
T 10 12.8 23.55 0.062 0.196 0.012 2300 765
T12 19.2 30.40 0.12 0.442 0.053 2300 1180
T 16 24.2 38.70 0.20 0.785 0.157 2300 1482
T 20 25.2 47.30 0.22 0.950 0.213 2300 1130
T 27 34.1 65.94 0.42 1.651 0.698 2300 1851
T 32 39.6 73.00 0.61 1.651 1.010 2300 2427
T 45 54.7 114.50 0.93 6.157 5.756 2300 2367
Chapter 5. Result and Conclusion 26
Appendix-2
SWG Dia with
enamel mm
Area of bare
conductor
mm2
R/Km
@20oC
ohms
Weight
Kg/km
45 0.086 0.003973 4340 0.0369
44 0.097 0.005189 3323 0.0481
43 0.109 0.006567 2626 0.0610
42 0.119 0.008107 2127 0.0750
41 0.132 0.009810 1758 0.0908
40 0.142 0.011675 1477 0.1079
39 0.152 0.013700 1258 0.1262
38 0.175 0.018240 945.2 0.1679
37 0.198 0.023430 735.9 0.2202
36 0.218 0.029270 589.1 0.2686
35 0.241 0.35750 482.2 0.3281
34 0.264 0.04289 402.0 0.3932
33 0.287 0.05067 340.3 0.4650
32 0.307 0.05910 291.7 0.5408
31 0.330 0.06818 252.9 0.6245
30 0.351 0.07791 221.3 0.7121
29 0.384 0.09372 184.0 0.8559
28 0.417 0.11100 155.3 1.0140
27 0.462 0.13630 126.5 1.2450
26 0.505 0.16420 105.0 1.4990
25 0.561 0.20270 85.1 1.8510
24 0.612 0.24520 70.3 2.2330
23 0.665 0.29190 59.1 2.6550
22 0.770 0.39730 43.4 3.6070
21 0.874 0.51890 33.2 4.7020
20 0.978 0.65670 23.3 59390
19 1.082 0.81070 21.3 7.3240
18 1.293 1.16700 14.8 10.5370
17 1.501 1.58900 10.8 14.3130
16 1.709 2.07500 8.3 18.6780
15 1.920 2.62700 6.6 23.6400
14 2.129 3.24300 5.3 29.1500
13 2.441 4.28900 4.0 38.5600
12 2.756 5.48000 3.1 49.2200
11 3.068 6.81800 2.5 61.0000
10 3.383 8.30200 2.1 74.0000
9 3.800 10.5100 1.6 94.0000
8 4.219 12.9700 1.3 116.0000
©2002 Fairchild Semiconductor Corporation IRF840 Rev. B
IRF840
8A, 500V, 0.850 Ohm, N-Channel Power MOSFET
This N-Channel enhancement mode silicon gate power field effect transistor is an advanced power MOSFET designed, tested, and guaranteed to withstand a specified level of energy in the breakdown avalanche mode of operation. All of these power MOSFETs are designed for applications such as switching regulators, switching converters, motor drivers, relay drivers, and drivers for high power bipolar switching transistors requiring high speed and low gate drive power. These types can be operated directly from integrated circuits.
Formerly developmental type TA17425.
Features
• 8A, 500V
• r
DS(ON)
= 0.850
Ω
• Single Pulse Avalanche Energy Rated
• SOA is Power Dissipation Limited
• Nanosecond Switching Speeds
• Linear Transfer Characteristics
• High Input Impedance
• Related Literature- TB334 “Guidelines for Soldering Surface Mount
Components to PC Boards”
Symbol
Packaging
JEDEC TO-220AB
TOP VIEW
Ordering Information
PART NUMBER PACKAGE BRAND
IRF840 TO-220AB IRF840
NOTE: When ordering, include the entire part number. G
D
S
SOURCEDRAIN
GATE
DRAIN(FLANGE)
Data Sheet January 2002
IRF840 Rev. B
Absolute Maximum Ratings
T
C
= 25
o
C, Unless Otherwise Specified
IRF840 UNITS
Drain to Source Voltage (Note 1) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .V
DS
500 VDrain to Gate Voltage (R
GS
= 20k
Ω)
(Note 1) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . V
DGR
500 VContinuous Drain Current . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . I
D
8.0 AT
C
= 100
o
C . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . I
D
5.1 APulsed Drain Current (Note 3) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . I
DM
32 AGate to Source Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .V
GS
±
20 VMaximum Power Dissipation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .P
D
125 WLinear Derating Factor . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1.0 W/
o
CSingle Pulse Avalanche Energy Rating (Note 4) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .E
AS
510 mJOperating and Storage Temperature . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . T
J
, T
STG
-55 to 150
o
CMaximum Temperature for Soldering
Leads at 0.063in (1.6mm) from Case for 10s. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . T
L
Package Body for 10s, See Techbrief 334 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . T
pkg
300260
o
C
o
C
CAUTION: Stresses above those listed in “Absolute Maximum Ratings” may cause permanent damage to the device. This is a stress only rating and operation of thedevice at these or any other conditions above those indicated in the operational sections of this specification is not implied.
NOTE:
1. T
J
= 25
o
C to 125
o
C.
Electrical Specifications
T
C
= 25
o
C, Unless Otherwise Specified
PARAMETER SYMBOL TEST CONDITIONS MIN TYP MAX UNITS
Drain to Source Breakdown Voltage BV
DSS
V
GS
= 0V, I
D
= 250
µ
A (Figure 10) 500 - - V
Gate to Threshold Voltage V
GS(TH)
V
GS
= V
DS
, I
D
= 250
µ
A 2.0 - 4.0 V
Zero-Gate Voltage Drain Current I
DSS
V
DS
= Rated BV
DSS
, V
GS
= 0V - - 25
µ
A
V
DS
= 0.8 x Rated BV
DSS
, V
GS
= 0V, T
J
= 125
o
C - - 250
µ
A
On-State Drain Current (Note 2) I
D(ON)
V
DS
> I
D(ON) x
r
DS(ON)MAX
, V
GS
= 10V 8.0 - - A
Gate to Source Leakage Current I
GSS
V
GS
=
±
20V - -
±
100 nA
Drain to Source On Resistance (Note 2) r
DS(ON)
V
GS
= 10V, I
D
= 4.4A (Figures 8, 9) - 0.8 0.85
Ω
Forward Transconductance (Note 2) g
fs
V
DS
≥
50V, I
D
= 4.4A (Figure 12) 4.9 7.4 - S
Turn-On Delay Time t
D(ON)
V
DD
=
250V, I
D
≈
8A, R
G
= 9.1
Ω
, R
L
= 30
Ω
MOSFET Switching Times are Essentially Independent of Operating Temperature.
- 15 21 ns
Rise Time t
r
- 21 35 ns
Turn-Off Delay Time t
D(OFF)
- 50 74 ns
Fall Time t
f
- 20 30 ns
Total Gate Charge (Gate to Source + Gate to Drain)
Q
g(TOT)
V
GS
= 10V, I
D
= 8A, V
DS
= 0.8 x Rated BV
DSS
I
g(REF)
= 1.5mA (Figure 14) Gate Charge is Essentially Independent of Operating Temperature
- 42 63 nC
Gate to Source Charge Q
gs
- 7.0 - nC
Gate to Drain “Miller” Charge Q
gd
- 22 - nC
Input Capacitance C
ISS
V
GS
= 0V, V
DS
= 25V, f = 1.0MHz (Figure 11) - 1225 - pF
Output Capacitance C
OSS
- 200 - pF
Reverse-Transfer Capacitance C
RSS
- 85 - pF
Internal Drain Inductance L
D
Measured from the Contact Screw on Tab to Center of Die
Modified MOSFET Symbol Showing the Internal Devices Inductances
- 3.5 - nH
Measured from the Drain Lead, 6mm (0.25in) from Package to Center of Die
- 4.5 - nH
Internal Source Inductance L
S
Measured from the Source Lead, 6mm (0.25in) from Header to Source Bonding Pad
- 7.5 - nH
Thermal Resistance Junction to Case R
θ
JC
- - 1.0
o
C/W
Thermal Resistance Junction to Ambient R
θ
JA
Free Air Operation - - 62.5
o
C/W
LS
LD
G
D
S
IRF840
©2002 Fairchild Semiconductor Corporation IRF840 Rev. B
Source to Drain Diode Specifications
PARAMETER SYMBOL TEST CONDITIONS MIN TYP MAX UNITS
Continuous Source to Drain Current I
SD
Modified MOSFET Symbol Showing the Integral Reverse P-N Junction Diode
- - 8.0 A
Pulse Source to Drain Current (Note 3) I
SDM
- - 32 A
Source to Drain Diode Voltage (Note 2) V
SD
T
J
= 25
o
C, I
SD
= 8.0A, V
GS
= 100A/
µ
s (Figure 13) - - 2.0 V
Reverse Recovery Time t
rr
T
J
= 25
o
C, I
SD
= 8.0A, dI
SD
/dt = 100A/
µ
s 210 475 970 ns
Reverse Recovered Charge Q
RR
T
J
= 25
o
C, I
SD
= 8.0A, dI
SD
/dt = 100A/
µ
s 2.0 4.6 8.2
µ
C
NOTES:
2. Pulse Test: Pulse width
≤
300
µ
s, duty cycle
≤
2%.
3. Repetitive Rating: Pulse width limited by Max junction temperature. See Transient Thermal Impedance curve (Figure 3).
4. V
DD
= 50V, starting T
J
= 25
o
C, L = 14mH, R
G = 25Ω, peak IAS = 8A.
Typical Performance Curves Unless Otherwise Specified
FIGURE 1. NORMALIZED POWER DISSIPATION vs CASE TEMPERATURE
FIGURE 2. MAXIMUM CONTINUOUS DRAIN CURRENT vs CASE TEMPERATURE
FIGURE 3. NORMALIZED MAXIMUM TRANSIENT THERMAL IMPEDANCE
G
D
S
0 50 100 1500
TC, CASE TEMPERATURE (oC)
PO
WE
R D
ISS
IPA
TIO
N M
ULT
IPL
IER
0.2
0.4
0.6
0.8
1.0
1.2
TC, CASE TEMPERATURE (oC)
50 75 10025 150
10
8
6
0
4
I D, D
RA
IN C
UR
RE
NT
(A
)
2
125
ZθJ
C, N
OR
MA
LIZ
ED
TR
AN
SIE
NT
1
10-210-5 10-4 10-3 0.1 1 10t1, RECTANGULAR PULSE DURATION (s)
10-3
0.1
10-2
DUTY FACTOR: D = t1/t2NOTES:
PEAK TJ = PDM x ZθJC x RθJC + TC
t2
PDM
t1t2
SINGLE PULSE
0.020.01
0.1
0.2
0.5
0.05
TH
ER
MA
L IM
PE
DA
NC
E
IRF840
IRF840 Rev. B
FIGURE 4. FORWARD BIAS SAFE OPERATING AREA FIGURE 5. OUTPUT CHARACTERISTICS
FIGURE 6. SATURATION CHARACTERISTICS FIGURE 7. TRANSFER CHARACTERISTICS
FIGURE 8. DRAIN TO SOURCE ON RESISTANCE vs VOLTAGE AND DRAIN CURRENT
FIGURE 9. NORMALIZED DRAIN TO SOURCE ON RESISTANCE vs JUNCTION TEMPERATURE
Typical Performance Curves Unless Otherwise Specified (Continued)
10
1 10 1020.1
I D,
DR
AIN
CU
RR
EN
T (
A)
VDS, DRAIN TO SOURCE VOLTAGE (V)
103
102
1
1ms
10ms
DC
100µs
10µs
OPERATION IN THISREGION IS LIMITEDBY rDS(ON)
TJ = MAX RATEDSINGLE PULSE
TC = 25oC
VDS, DRAIN TO SOURCE VOLTAGE (V)
50 100 150 2000
15
12
9
0
6
I D, D
RA
IN C
UR
RE
NT
(A
)
PULSE DURATION = 80µs
3
250
VGS = 5.0V
VGS = 6.0V
VGS = 10V
VGS = 4.0VVGS = 4.5V
VGS = 5.5V
DUTY CYCLE = 0.5% MAX
VDS, DRAIN TO SOURCE VOLTAGE (V)3 6 9 120 15
15
12
9
0
6
I D, D
RA
IN C
UR
RE
NT
(A
)
3
VGS = 10V
VGS = 4.0V
VGS = 6.0V
VGS = 5.5V
VGS = 4.5V
VGS = 5.0V
PULSE DURATION = 80µsDUTY CYCLE = 0.5% MAX
I SD
(ON
), D
RA
IN T
O S
OU
RC
E
VSD, GATE TO SOURCE VOLTAGE (V)
100
10
0.1
0 2 4 6 8 10
TJ = 150oC TJ = 25oC
1
0.01
CU
RR
EN
T (
A)
PULSE DURATION = 80µsDUTY CYCLE = 0.5% MAXVDS ≥ 50V
TC, CASE TEMPERATURE (oC)8 16 240 40
10
8
6
0
4
2
32
VGS = 20V
VGS = 10V
r DS
(ON
), D
RA
IN T
O S
OU
RC
EO
N R
ES
ISTA
NC
E (
Ω)
PULSE DURATION = 80µsDUTY CYCLE = 0.5% MAX
20
3.0
1.8
0.6
100
TJ, JUNCTION TEMPERATURE (oC)
NO
RM
AL
IZE
D D
RA
IN T
O S
OU
RC
E
2.4
1.2
0140
ON
RE
SIS
TAN
CE
VO
LTA
GE
-40 60 16012080400-60 -20
PULSE DURATION = 80µsDUTY CYCLE = 0.5% MAXID = 4.4A, VGS = 10V
IRF840
©2002 Fairchild Semiconductor Corporation IRF840 Rev. B
FIGURE 10. NORMALIZED DRAIN TO SOURCE BREAKDOWN VOLTAGE vs JUNCTION TEMPERATURE
FIGURE 11. CAPACITANCE vs DRAIN TO SOURCE VOLTAGE
FIGURE 12. TRANSCONDUCTANCE vs DRAIN CURRENT FIGURE 13. SOURCE TO DRAIN DIODE VOLTAGE
FIGURE 14. GATE TO SOURCE VOLTAGE vs GATE CHARGE
Typical Performance Curves Unless Otherwise Specified (Continued)
20
1.25
1.05
0.85
100
TJ, JUNCTION TEMPERATURE (oC)
1.15
0.95
0.75140-40 60 16012080400-60 -20
ID = 250µA
NO
RM
AL
IZE
D D
RA
IN T
O S
OU
RC
EB
RE
AK
DO
WN
VO
LTA
GE
1
C, C
APA
CIT
AN
CE
(p
F)
VDS, DRAIN TO SOURCE VOLTAGE (V)
3000
2400
1800
1200
600
02 5 10210
CISS
52
VGS = 0V, f = 1MHzCISS = CGS + CGDCRSS = CGDCOSS ≈ CDS + CGD
COSS
CRSS
ID, DRAIN CURRENT (A)3 6 9 120 15
15
12
9
0
6
gfs
, TR
AN
SC
ON
DU
CTA
NC
E (
S)
3
TJ = 25oC
TJ = 150oC
PULSE DURATION = 80µsDUTY CYCLE = 0.5% MAXVDS ≥ 50V
I SD
, SO
UR
CE
TO
DR
AIN
CU
RR
EN
T (
A)
VSD, SOURCE TO DRAIN VOLTAGE (V)
10
0 0.3 0.6 0.9 1.5
1.0
TJ = 150oC
1.20.1
100
TJ = 25oC
PULSE DURATION = 80µsDUTY CYCLE = 0.5% MAX
Qg, GATE CHARGE (nC)
12 24 36 480 60
20
8
VG
S, G
AT
E T
O S
OU
RC
E V
OLT
AG
E (
V)
16
12
0
ID = 8A
4
VDS = 250V
VDS = 100V
VDS = 400V
IRF840
IRF840 Rev. B
Test Circuits and Waveforms
FIGURE 15. UNCLAMPED ENERGY TEST CIRCUIT FIGURE 16. UNCLAMPED ENERGY WAVEFORMS
FIGURE 17. SWITCHING TIME TEST CIRCUIT FIGURE 18. RESISTIVE SWITCHING WAVEFORMS
FIGURE 19. GATE CHARGE TEST CIRCUIT FIGURE 20. GATE CHARGE WAVEFORMS
tP
VGS
0.01Ω
L
IAS
+
-
VDS
VDDRG
DUT
VARY tP TO OBTAIN
REQUIRED PEAK IAS
0V
VDD
VDS
BVDSS
tP
IAS
tAV
0
VGS
RL
RG
DUT
+
-VDD
tON
td(ON)
tr
90%
10%
VDS90%
10%
tf
td(OFF)
tOFF
90%
50%50%
10%PULSE WIDTH
VGS
0
0
0.3µF
12VBATTERY 50kΩ
VDS
S
DUT
D
G
Ig(REF)0
(ISOLATEDVDS
0.2µF
CURRENTREGULATOR
ID CURRENTSAMPLING
IG CURRENTSAMPLING
SUPPLY)
RESISTOR RESISTOR
SAME TYPEAS DUT
Qg(TOT)
Qgd
Qgs
VDS
0
VGS
VDD
Ig(REF)
0
IRF840
DISCLAIMER
FAIRCHILD SEMICONDUCTOR RESERVES THE RIGHT TO MAKE CHANGES WITHOUT FURTHERNOTICE TO ANY PRODUCTS HEREIN TO IMPROVE RELIABILITY, FUNCTION OR DESIGN. FAIRCHILDDOES NOT ASSUME ANY LIABILITY ARISING OUT OF THE APPLICATION OR USE OF ANY PRODUCTOR CIRCUIT DESCRIBED HEREIN; NEITHER DOES IT CONVEY ANY LICENSE UNDER ITS PATENTRIGHTS, NOR THE RIGHTS OF OTHERS.
TRADEMARKS
The following are registered and unregistered trademarks Fairchild Semiconductor owns or is authorized to use and isnot intended to be an exhaustive list of all such trademarks.
LIFE SUPPORT POLICY
FAIRCHILD’S PRODUCTS ARE NOT AUTHORIZED FOR USE AS CRITICAL COMPONENTS IN LIFE SUPPORTDEVICES OR SYSTEMS WITHOUT THE EXPRESS WRITTEN APPROVAL OF FAIRCHILD SEMICONDUCTOR CORPORATION.As used herein:1. Life support devices or systems are devices orsystems which, (a) are intended for surgical implant intothe body, or (b) support or sustain life, or (c) whosefailure to perform when properly used in accordancewith instructions for use provided in the labeling, can bereasonably expected to result in significant injury to theuser.
2. A critical component is any component of a lifesupport device or system whose failure to perform canbe reasonably expected to cause the failure of the lifesupport device or system, or to affect its safety oreffectiveness.
PRODUCT STATUS DEFINITIONS
Definition of Terms
Datasheet Identification Product Status Definition
Advance Information
Preliminary
No Identification Needed
Obsolete
This datasheet contains the design specifications forproduct development. Specifications may change inany manner without notice.
This datasheet contains preliminary data, andsupplementary data will be published at a later date.Fairchild Semiconductor reserves the right to makechanges at any time without notice in order to improvedesign.
This datasheet contains final specifications. FairchildSemiconductor reserves the right to make changes atany time without notice in order to improve design.
This datasheet contains specifications on a productthat has been discontinued by Fairchild semiconductor.The datasheet is printed for reference information only.
Formative orIn Design
First Production
Full Production
Not In Production
OPTOLOGIC™OPTOPLANAR™PACMAN™POP™Power247™PowerTrenchQFET™QS™QT Optoelectronics™Quiet Series™SILENT SWITCHER
FASTFASTr™FRFET™GlobalOptoisolator™GTO™HiSeC™ISOPLANAR™LittleFET™MicroFET™MicroPak™MICROWIRE™
Rev. H4
ACEx™Bottomless™CoolFET™CROSSVOLT™DenseTrench™DOME™EcoSPARK™E2CMOSTM
EnSignaTM
FACT™FACT Quiet Series™
SMART START™STAR*POWER™Stealth™SuperSOT™-3SuperSOT™-6SuperSOT™-8SyncFET™TinyLogic™TruTranslation™UHC™UltraFET
STAR*POWER is used under license
VCX™
This datasheet has been download from:
www.datasheetcatalog.com
Datasheets for electronics components.
BYQ28E, BYQ28EF, BYQ28EB, UG10DCT, UGF10DCT, UGB10DCT SeriesVishay Semiconductorsformerly General Semiconductor
Document Number 88549 www.vishay.com25-Jun-03 1
Dual Ultrafast Soft Recovery RectifierReverse Voltage 100 to 200V Forward Current 10A
Reverse Recovery Time 20ns
0.08(2.032)
0.24(6.096)
0.42(10.66)
0.63(17.02)
0.12(3.05)
0.33(8.38)
Mounting Pad Layout TO-263AB 0.380 (9.65)
0.411 (10.45)
0.320 (8.13)
0.360 (9.14)
0.591 (15.00)
0.624 (15.85)
1 2
0.245 (6.22) MIN
K
K
0.160 (4.06)
0.190 (4.83)
0.045 (1.14)
0.055 (1.40)
0.014 (0.36)
0.021 (0.53)
0.110 (2.79)
0.140 (3.56)
0.090 (2.29)
0.110 (2.79)
0.047 (1.19)
0.055 (1.40)
PIN 1
PIN 2 K - HEATSINK
0-0.01 (0-0.254)
0.027 (0.686)
0.037 (0.940)
0.105 (2.67)
0.095 (2.41)0.205 (5.20)
0.195 (4.95)
1 3
PIN
2
0.060 (1.52)
0.405 (10.27)0.383 (9.72)
0.191 (4.85)0.171 (4.35)
0.600 (15.5)0.580 (14.5)
0.560 (14.22)0.530 (13.46)
0.037 (0.94)0.027 (0.69)
0.140 (3.56)0.130 (3.30)
0.350 (8.89)0.330 (8.38)
0.188 (4.77)0.172 (4.36)
0.110 (2.80)0.100 (2.54)
0.131 (3.39)0.122 (3.08)
0.110 (2.80)0.100 (2.54)
0.022 (0.55)0.014 (0.36)
DIA.DIA.
0.676 (17.2)0.646 (16.4)
0.205 (5.20)0.195 (4.95)
0.105 (2.67)0.095 (2.41)
PIN 2PIN 1
PIN 3
ITO-220AB (BYQ28EF, UGF10 Series)
TO-220AB (BYQ28E, UG10 Series)
Dimensions in inchesand (millimeters)
TO-263AB (BYQ28EB, UGB10 Series)
1 2 3PIN
0.185 (4.70)
0.175 (4.44)
0.055 (1.39)0.045 (1.14)
0.145 (3.68)0.135 (3.43)
0.350 (8.89)0.330 (8.38)
0.560 (14.22)0.530 (13.46)
0.022 (0.56)0.014 (0.36)
0.110 (2.79)0.100 (2.54)
0.603 (15.32)0.573 (14.55)
CASE
1.148 (29.16)1.118 (28.40)
PIN 2
0.154 (3.91)
0.148 (3.74)
0.113 (2.87)0.103 (2.62)
0.160 (4.06)
0.140 (3.56)
0.410 (10.41)0.390 (9.91)
0.635 (16.13)
0.625 (15.87)
0.415 (10.54) MAX.
0.370 (9.40)0.360 (9.14)
PIN 1
PIN 3
0.028 (0.70)0.104 (2.65)0.096 (2.45)
0.035 (0.90)
0.205 (5.20)0.195 (4.95)
0.105 (2.67)
0.095 (2.41)
Features• Plastic package has Underwriters Laboratories
Flammability Classification 94V-0• High reverse energy capability• Excellent high temperature switching• High temperature soldering guaranteed: 250°C/10
seconds at terminals• Glass passivated chip junction• Soft recovery characteristics
Mechanical DataCase: JEDEC TO-220AB, ITO-220AB & TO-263AB molded plastic body
Terminals: Plated leads, solderable per MIL-STD-750, Method 2026
Polarity: As marked Mounting Position: Any
Mounting Torque: 10 in-lbs maximum
Weight: 0.08 oz., 2.24 g
BYQ28E, BYQ28EF, BYQ28EB, UG10DCT, UGF10DCT, UGB10DCT SeriesVishay Semiconductorsformerly General Semiconductor
www.vishay.com Document Number 885492 25-Jun-03
Maximum Ratings (TC = 25°C unless otherwise noted) UG10BCT UG10CCT UG10DCT
Parameter Symbol BYQ28E-100 BYQ28E-150 BYQ28E-200 Unit
Maximum repetitive peak reverse voltage VRRM 100 150 200 V
Working peak reverse voltage VRWM 100 150 200 V
Maximum DC blocking voltage VDC 100 150 200 V
Maximum average forward rectified current Total device 10at TC = 100°C Per leg IF(AV) 5 A
Peak forward surge current8.3ms single half sine-wave superimposed IFSM 55 Aon rated load (JEDEC Method) per leg
Repetitive peak reverse current per leg at tp = 100µs IRRM 0.2 A
Electrostatic discharge capacitor voltage,Human body model: C = 250pF, R = 1.5kΩ VC 8 KV
Operating junction and storage temperature range TJ, TSTG –40 to +150 °C
Non-repetitive peak reverse current per leg IRSM 0.2 Aat tp= 100µs
RMS Isolation voltage (BYQ28EF, UGF types) 4500 (NOTE 1)
from terminals to heatsink with t = 1 second, RH ≤ 30% VISOL 3500 (NOTE 2) V1500 (NOTE 3)
Electrical Characteristics (TC = 25°C unless otherwise noted)
Parameter Symbol Value Unit
Maximum instantaneous forward voltage per leg (Note 4)
at IF = 10A, TJ = 25°C 1.25at IF = 5A, TJ = 25°C VF 1.10 Vat IF = 5A, TJ = 150°C 0.895
Maximum reverse current per leg TJ = 25°C 10at working peak reverse voltage (Note 4) TJ = 100°C IR 200 µA
Maximum reverse recovery time per leg at IF = 1.0A, di/dt = 100A/µs, VR = 30V, Irr = 0.1IRM
trr 25 ns
Maximum reverse recovery time per leg at IF = 0.5A, IR = 1.0A, Irr = 0.25A trr 20 ns
Maximum stored charge per legIF = 2A, di/dt = 20A/µs, VR = 30V, Irr = 0.1IRM
Qrr 9 nC
Thermal Characteristics (TC = 25°C unless otherwise noted) UG10 UGF10 UGB10
Parameter Symbol BYQ28E BYQ28EF BYQ28EB Unit
Typical thermal resistance — junction to ambient RΘJA 50 55 50 °C/Wper leg — junction to case RΘJC 4.5 6.7 4.5 °C/W
Notes:(1) Clip mounting (on case), where lead does not overlap heatsink with 0.110” offset(2) Clip mounting (on case), where leads do overlap heatsink(3) Screw mounting with 4-40 screw, where washer diameter is ≤ 4.9 mm (0.19”)(4) Pulse test: 300µs pulse width, 1% duty cycle
BYQ28E(F,B,D) Series, UG10(F,B,D)10BCT thru UG10(F,B,D)DCTVishay Semiconductorsformerly General Semiconductor
Document Number 88549 www.vishay.com25-Jun-03 3
Ratings and Characteristic Curves (TA = 25°C unless otherwise noted)
I F –
Inst
anta
neou
s F
orw
ard
Cur
rent
(A
) 100
10
I R –
Inst
anta
neou
s R
ever
se C
urre
nt (
µA)
Typical Reverse Characteristics Per Leg
1.0
0.1
0.01
Forward Current Derating Curve
0
5
15
0 50 100 150
10
Ave
rage
For
war
d C
urre
nt (
A)
Pea
k F
orw
ard
Sur
ge C
urre
nt (
A)
Number of Cycles at 60 HZ
Maximum Non-Repetitive Peak Forward Surge Current Per Leg
1
10
100
1 10 100
Case Temperature (°C)
1.0
10
100
1000
0.1
TJ = 125°C
100°C
25°C
Resistive or Inductive Load
TJ = 25°C
TJ = 125°C
1 10 100
10
100
10.1
Reverse Voltage (V)
TJ = 125°Cf = 1.0 MHZ
Vsig = 50mVp-p
0.2 0.4 0.8 1.40.6 1.0 1.2
Pulse Width = 300µs1% Duty Cycle
TC = 105°C8.3ms Single Half Sine-Wave(JEDEC Method)
TJ = 100°C
Reverse Switching Characteristics Per Leg
0
50
25 50 75 100 125
10
20
30
Sto
red
Cha
rge/
Rev
erse
Rec
over
y T
ime
(nC
/ns)
40
@5A, 50A/µs
@2A, 20A/µs
@2A, 20A/µs
@1A, 100A/µs
@5A, 50A/µs
20 10040 60 80
Percent of Rated Peak Reverse Voltage (%)
Typical Junction Capacitance Per Leg
pF –
Jun
ctio
n C
apac
itanc
eTypical Instantaneous
Forward Characteristics Per Leg
Instantaneous Forward Voltage (V)
Junction Temperature (°C)
@1A, 100A/µs
trrQrr
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
1POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
Complete Pulse-Width Modulation (PWM)Power-Control Circuitry
Uncommitted Outputs for Single-Ended orPush-Pull Applications
Low Standby Current . . . 8 mA Typ
Interchangeable With Industry StandardSG2524 and SG3524
description/ordering information
The SG2524 and SG3524 incorporate all thefunctions required in the construction of aregulating power supply, inverter, or switchingregulator on a single chip. They also can be usedas the control element for high-power-outputapplications. The SG2524 and SG3524 weredesigned for switching regulators of either polarity, transformer-coupled dc-to-dc converters, transformerlessvoltage doublers, and polarity-converter applications employing fixed-frequency, pulse-width modulation(PWM) techniques. The complementary output allows either single-ended or push-pull application. Each deviceincludes an on-chip regulator, error amplifier, programmable oscillator, pulse-steering flip-flop, two uncommittedpass transistors, a high-gain comparator, and current-limiting and shutdown circuitry.
ORDERING INFORMATION
TINPUT
REGULATION PACKAGE† ORDERABLE TOP-SIDETA REGULATION
MAX (mV)PACKAGE† ORDERABLE
PART NUMBERTOP-SIDEMARKING
PDIP (N) Tube of 25 SG3524N SG3524N
0°C to 70°C 30 SOIC (D)Tube of 40 SG3524D
SG35240°C to 70°C 30 SOIC (D)Reel of 2500 SG3524DR
SG3524
SOP (NS) Reel of 2000 SG3524NSR SG3524
PDIP (N) Tube of 25 SG2524N SG2524N
–25°C to 85°C 20SOIC (D)
Tube of 40 SG2524DSG2524SOIC (D)
Reel of 2500 SG2524DRSG2524
† Package drawings, standard packing quantities, thermal data, symboliztion, and PCB design guidelines areavailable at www.ti.com/sc/package.
Copyright 2003, Texas Instruments Incorporated ! "#$ ! %#&'" ( $)(#" ! " !%$"" ! %$ *$ $! $+! ! #$ !! (( , -) (#" %"$!!. ($! $"$!!'- "'#($ $! . '' %$ $!)
Please be aware that an important notice concerning availability, standard warranty, and use in critical applications ofTexas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet.
1
2
3
4
5
6
7
8
16
15
14
13
12
11
10
9
IN–IN+
OSC OUTCURR LIM+CURR LIM–
RTCT
GND
REF OUTVCCEMIT 2COL 2COL 1EMIT 1SHUTDOWNCOMP
SG2524 . . . D OR N PACKAGESG3524 . . . D, N, OR NS PACKAGE
(TOP VIEW)
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
2 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
functional block diagram
T COL 2
OSC OUTEMIT 2
EMIT 1
COL 1
Vref
ReferenceRegulator
Comparator
Oscillator
SHUTDOWN
Error Amplifier
1
2
9
4
5CURR LIM–
CURR LIM+
GND8
10
+
–
+
–
NOTE A: Resistor values shown are nominal.
12
1113
143
IN–
IN+
COMP
1 kΩ10 kΩ
15
RT
CT
REF OUT16
6
7
Vref
Vref
Vref
Vref
VCC
Vref
absolute maximum ratings over operating free-air temperature range (unless otherwise noted)†
Supply voltage, VCC (see Notes 1 and 2) 40 V. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Collector output current, ICC 100 mA. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Reference output current, IO(ref) 50 mA. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Current through CT terminal –5 mA. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Operating virtual junction temperature, TJ 150°C. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Package thermal impedance, θJA (see Notes 3 and 4): D package 73°C/W. . . . . . . . . . . . . . . . . . . . . . . . . . .
N package 67°C/W. . . . . . . . . . . . . . . . . . . . . . . . . . . . NS package 64°C/W. . . . . . . . . . . . . . . . . . . . . . . . . . .
Lead temperature 1,6 mm (1/16 inch) from case for 10 seconds 260°C. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Storage temperature range, Tstg –65°C to 150°C. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
† Stresses beyond those listed under “absolute maximum ratings” may cause permanent damage to the device. These are stress ratings only, andfunctional operation of the device at these or any other conditions beyond those indicated under “recommended operating conditions” is notimplied. Exposure to absolute-maximum-rated conditions for extended periods may affect device reliability.
NOTES: 1. All voltage values are with respect to network ground terminal.2. The reference regulator may be bypassed for operation from a fixed 5-V supply by connecting the VCC and reference output
(REF OUT) pin both to the supply voltage. In this configuration, the maximum supply voltage is 6 V.3. Maximum power dissipation is a function of TJ(max), θJA, and TA. The maximum allowable power dissipation at any allowable ambient
temperature is PD = (TJ(max) – TA)/θJA. Operation at the absolute maximum TJ of 150°C can impact reliability.4. The package thermal impedance is calculated in accordance with JESD 51-7.
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
3POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
recommended operating conditionsMIN MAX UNIT
VCC Supply voltage 8 40 V
Reference output current 0 50 mA
Current through CT terminal –0.03 –2 mA
RT Timing resistor 1.8 100 kΩ
CT Timing capacitor 0.001 0.1 µF
TA Operating free air temperatureSG2524 –25 85
°CTA Operating free-air temperatureSG3524 0 70
°C
electrical characteristics over recommended operating free-air temperature range, VCC = 20 V,f = 20 kHz (unless otherwise noted)
reference section
PARAMETER TEST CONDITIONS†SG2524 SG3524
UNITPARAMETER TEST CONDITIONS†MIN TYP‡ MAX MIN TYP‡ MAX
UNIT
Output voltage 4.8 5 5.2 4.6 5 5.4 V
Input regulation VCC = 8 V to 40 V 10 20 10 30 mV
Ripple rejection f = 120 Hz 66 66 dB
Output regulation IO = 0 mA to 20 mA 20 50 20 50 mV
Output voltage change with temperature TA = MIN to MAX 0.3% 1% 0.3% 1%
Short-circuit output current§ Vref = 0 100 100 mA
† For conditions shown as MIN or MAX, use the appropriate value specified under recommended operating conditions.‡ All typical values, except for temperature coefficients, are at TA = 25°C§ Standard deviation is a measure of the statistical distribution about the mean, as derived from the formula:
N
n1
(xn X)2
N 1
oscillator section
PARAMETER TEST CONDITIONS† MIN TYP‡ MAX UNIT
fosc Oscillator frequency CT = 0.001 µF, RT = 2 kΩ 450 kHz
Standard deviation of frequency§ All values of voltage, temperature, resistance,and capacitance constant
5%
∆fFrequency change with voltage VCC = 8 V to 40 V, TA = 25°C 1%
∆fosc Frequency change with temperature TA = MIN to MAX 2%
Output amplitude at OSC OUT TA = 25°C 3.5 V
tw Output pulse duration (width) at OSC OUT CT = 0.01 µF, TA = 25°C 0.5 µs
† For conditions shown as MIN or MAX, use the appropriate value specified under recommended operating conditions.‡ All typical values, except for temperature coefficients, are at TA = 25°C§ Standard deviation is a measure of the statistical distribution about the mean, as derived from the formula:
N
n1
(xn X)2
N 1
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
4 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
error amplifier section
PARAMETERTEST SG2524 SG3524
UNITPARAMETERTEST
CONDITIONS† MIN TYP‡ MAX MIN TYP‡ MAXUNIT
VIO Input offset voltage VIC = 2.5 V 0.5 5 2 10 mV
IIB Input bias current VIC = 2.5 V 2 10 2 10 µA
Open-loop voltage amplification 72 80 60 80 dB
VICR Common-mode input voltage range TA = 25°C1.8 to
3.41.8 to
3.4V
CMMR Common-mode rejection ratio 70 70 dB
B1 Unity-gain bandwidth 3 3 MHz
Output swing TA = 25°C 0.5 3.8 0.5 3.8 V
† For conditions shown as MIN or MAX, use the appropriate value specified under recommended operating conditions.‡ All typical values, except for temperature coefficients, are at TA = 25°C
output sectionPARAMETER TEST CONDITIONS† MIN TYP‡ MAX UNIT
V(BR)CE Collector-emitter breakdown voltage 40 V
Collector off-state current VCE = 40 V 0.01 50 µA
Vsat Collector-emitter saturation voltage IC = 50 mA 1 2 V
VO Emitter output voltage VC = 20 V, IE = –250 µA 17 18 V
tr Turn-off voltage rise time RC = 2 kΩ 0.2 µs
tf Turn-on voltage fall time RC = 2 kΩ 0.1 µs
† For conditions shown as MIN or MAX, use the appropriate value specified under recommended operating conditions.‡ All typical values, except for temperature coefficients, are at TA = 25°C.
comparator sectionPARAMETER TEST CONDITIONS† MIN TYP‡ MAX UNIT
Maximum duty cycle, each output 45%
V Inp t threshold oltage at COMPZero duty cycle 1
VVIT Input threshold voltage at COMPMaximum duty cycle 3.5
V
IIB Input bias current –1 µA
† For conditions shown as MIN or MAX, use the appropriate value specified under recommended operating conditions.‡ All typical values, except for temperature coefficients, are at TA = 25°C.
current limiting sectionPARAMETER TEST CONDITIONS† MIN TYP‡ MAX UNIT
VI Input voltage range (either input) –1 to1 V
V(SENSE) Sense voltage at TA = 25°CV(IN ) V(IN ) ≥ 50 mV V(COMP) 2 V
175 200 225 mV
Temperature coefficient of sense voltageV(IN+) – V(IN–) ≥ 50 mV, V(COMP) = 2 V
0.2 mV/°C‡ All typical values, except for temperature coefficients, are at TA = 25°C.
total devicePARAMETER TEST CONDITIONS MIN TYP‡ MAX UNIT
Ist Standby currentVCC = 40 V, IN–, CURR LIM+, CT, GND, COMP, EMIT 1, EMIT 2 grounded,IN+ at 2 V, All other inputs and outputs open
8 10 mA
‡ All typical values, except for temperature coefficients, are at TA = 25°C.
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
5POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
PARAMETER MEASUREMENT INFORMATION
0.1 µF
2 kΩ
10 kΩ
RT
1 W2 kΩ
8
4
2
1
9
6
7
10
11
14
16
3
12
13
(Open)
Outputs
VCC = 8 V to 40 V
15
SHUTDOWN
CT
RT
COMP
IN–
IN+
CURR LIM+ COL 2
COL 1
OSC OUT
REF OUT
EMIT 2
EMIT 1
GND
SG2524 or SG3524
VCC
CT
2 kΩ
1 W2 kΩ
2 kΩ10 kΩ
1 kΩ
5CURR LIM–
VREF
VREF
Figure 1. General Test Circuit
≈0 V
≈VCC
VOLTAGE WAVEFORMS
90%
10%10%
90%
trtf
TEST CIRCUIT
Circuit Under Test
Output
2 kΩ
VCC
Output
Figure 2. Switching Times
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
6 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
TYPICAL CHARACTERISTICS
Frequency – Hz
–10
0
10
20
30
40
50
60
70
80
90
Op
en-L
oo
p V
olt
age
Am
plif
icat
ion
of
Err
or
Am
plif
ier
– d
B
10 M1 M100 k10 k1 k100
RL is resistance from COMP to ground
ÏÏÏÏÏÏÏÏÏÏ
RL = 300 kΩ
ÏÏÏÏRL = 1 MΩ
ÏÏÏÏÏÏÏÏÏÏ
RL = 100 kΩ
ÏÏÏÏÏÏÏÏ
RL = 30 kΩ
OPEN-LOOP VOLTAGE AMPLIFICATIONOF ERROR AMPLIFIER
vsFREQUENCY
VCC = 20 VTA = 25°C
RL = ∞
Figure 3
1
– O
scill
ato
r F
req
uen
cy –
Hz
RT – Timing Resistance – kΩ
20 40 1007010742
OSCILLATOR FREQUENCYvs
TIMING RESISTANCE
VCC = 20 VTA = 25°C
1M
400 k
100 k
40 k
10 k
4 k
1 k
400
100
CT = 0.1 µF
CT = 0.01 µF
CT = 0.03 µF
CT = 0.003 µF
CT = 0
f osc
CT = 0.001 µF
Figure 4
OUTPUT DEAD TIMEvs
TIMING CAPACITANCE
1
10
4
0.001 0.01
Ou
tpu
t D
ead
Tim
e –
0.004 0.10.040.1
0.4
µs
CT – Timing Capacitance – µF
Figure 5
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
7POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
PRINCIPLES OF OPERATION†
The SG2524 is a fixed-frequency pulse-width-modulation (PWM) voltage-regulator control circuit. The regulatoroperates at a fixed frequency that is programmed by one timing resistor, RT, and one timing capacitor, CT. RTestablishes a constant charging current for CT. This results in a linear voltage ramp at CT, which is fed to thecomparator, providing linear control of the output pulse duration (width) by the error amplifier. The SG2524 containsan onboard 5-V regulator that serves as a reference, as well as supplying the SG2524 internal regulator controlcircuitry. The internal reference voltage is divided externally by a resistor ladder network to provide a reference withinthe common-mode range of the error amplifier as shown in Figure 6, or an external reference can be used. The outputis sensed by a second resistor divider network and the error signal is amplified. This voltage is then compared to thelinear voltage ramp at CT. The resulting modulated pulse out of the high-gain comparator then is steered to theappropriate output pass transistor (Q1 or Q2) by the pulse-steering flip-flop, which is synchronously toggled by theoscillator output. The oscillator output pulse also serves as a blanking pulse to ensure both outputs are never onsimultaneously during the transition times. The duration of the blanking pulse is controlled by the value of CT. Theoutputs may be applied in a push-pull configuration in which their frequency is one-half that of the base oscillator, orparalleled for single-ended applications in which the frequency is equal to that of the oscillator. The output of the erroramplifier shares a common input to the comparator with the current-limiting and shut-down circuitry and can beoverridden by signals from either of these inputs. This common point is pinned out externally via the COMP pin, whichcan be employed to either control the gain of the error amplifier or to compensate it. In addition, the COMP pin canbe used to provide additional control to the regulator.
APPLICATION INFORMATION†
oscillator
The oscillator controls the frequency of the SG2524 and is programmed by RT and CT as shown in Figure 4.
f 1.30RT CT
where: RT is in kΩCT is in µFf is in kHz
Practical values of CT fall between 0.001 µF and 0.1 µF. Practical values of RT fall between 1.8 kΩ and 100 kΩ.This results in a frequency range typically from 130 Hz to 722 kHz.
blanking
The output pulse of the oscillator is used as a blanking pulse at the output. This pulse duration is controlled bythe value of CT as shown in Figure 5. If small values of CT are required, the oscillator output pulse duration canbe maintained by applying a shunt capacitance from OSC OUT to ground.
synchronous operation
When an external clock is desired, a clock pulse of approximately 3 V can be applied directly to the oscillatoroutput terminal. The impedance to ground at this point is approximately 2 kΩ. In this configuration, RTCT mustbe selected for a clock period slightly greater than that of the external clock.
† Throughout these discussions, references to the SG2524 apply also to the SG3524.
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
8 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
APPLICATION INFORMATION†
synchronous operation (continued)
If two or more SG2524 regulators are operated synchronously, all oscillator output terminals must be tiedtogether. The oscillator programmed for the minimum clock period is the master from which all the otherSG2524s operate. In this application, the CTRT values of the slaved regulators must be set for a periodapproximately 10% longer than that of the master regulator. In addition, CT (master) = 2 CT (slave) to ensurethat the master output pulse, which occurs first, has a longer pulse duration and, subsequently, resets the slaveregulators.
voltage reference
The 5-V internal reference can be employed by use of an external resistor divider network to establish areference common-mode voltage range (1.8 V to 3.4 V) within the error amplifiers (see Figure 6), or an externalreference can be applied directly to the error amplifier. For operation from a fixed 5-V supply, the internalreference can be bypassed by applying the input voltage to both the VCC and VREF terminals. In thisconfiguration, however, the input voltage is limited to a maximum of 6 V.
To NegativeOutput Voltage
REF OUT
5 kΩR1
To PositiveOutput Voltage
R25 kΩ
REF OUT
+
–
+
–
5 kΩ
5 kΩ
R2
R1
VO 2.5 V R1 R2R1
VO 2.5 V 1 R2R1
2.5 V 2.5 V
Figure 6. Error-Amplifier Bias Circuits
error amplifier
The error amplifier is a differential-input transconductance amplifier. The output is available for dc gain controlor ac phase compensation. The compensation node (COMP) is a high-impedance node (RL = 5 MΩ). The gainof the amplifier is AV = (0.002 Ω–1)RL and easily can be reduced from a nominal 10,000 by an external shuntresistance from COMP to ground. Refer to Figure 3 for data.
compensation
COMP, as previously discussed, is made available for compensation. Since most output filters introduce oneor more additional poles at frequencies below 200 Hz, which is the pole of the uncompensated amplifier,introduction of a zero to cancel one of the output filter poles is desirable. This can be accomplished best witha series RC circuit from COMP to ground in the range of 50 kΩ and 0.001 µF. Other frequencies can be canceledby use of the formula f ≈ 1/RC.
† Throughout these discussions, references to the SG2524 apply also to the SG3524.
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
9POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
APPLICATION INFORMATION†
shutdown circuitry
COMP also can be employed to introduce external control of the SG2524. Any circuit that can sink 200 µA canpull the compensation terminal to ground and, thus, disable the SG2524.
In addition to constant-current limiting, CURR LIM+ and CURR LIM– also can be used in transformer-coupledcircuits to sense primary current and shorten an output pulse should transformer saturation occur. CURR LIM–also can be grounded to convert CURR LIM+ into an additional shutdown terminal.
current limiting
A current-limiting sense amplifier is provided in the SG2524. The current-limiting sense amplifier exhibits athreshold of 200 mV ±25 mV and must be applied in the ground line since the voltage range of the inputs is limitedto 1 V to –1 V. Caution should be taken to ensure the –1-V limit is not exceeded by either input, otherwise,damage to the device may result.
Foldback current limiting can be provided with the network shown in Figure 7. The current-limit schematic isshown in Figure 8.
VO
RsR2
R1EMIT 2
EMIT 1
SG2524
IO(max) 1
Rs200 mV
VO R2
R1 R2
IOS 200 mV
Rs
CURR LIM+
CURR LIM–
11
14
5
4
Figure 7. Foldback Current Limiting for Shorted Output Conditions
Constant-Current Source
CURR LIM+
COMP CT
Comparator
Error Amplifier
CURR LIM–
Figure 8. Current-Limit Schematic
† Throughout these discussions, references to the SG2524 apply also to the SG3524.
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
10 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
APPLICATION INFORMATION†
output circuitry
The SG2524 contains two identical npn transistors, the collectors and emitters of which are uncommitted. Eachtransistor has antisaturation circuitry that limits the current through that transistor to a maximum of 100 mA forfast response.
general
There are a wide variety of output configurations possible when considering the application of the SG2524 asa voltage-regulator control circuit. They can be segregated into three basic categories:
Capacitor-diode-coupled voltage multipliers Inductor-capacitor-implemented single-ended circuits Transformer-coupled circuits
Examples of these categories are shown in Figures 9, 10, and 11, respectively. Detailed diagrams of specificapplications are shown in Figures 12–15.
D1
VI
VO
VI < VO
VI
D1
VO
VI > VO
D1
VI
–VO
| +VI | > | – VO |
Figure 9. Capacitor-Diode-Coupled Voltage-Multiplier Output Stages
† Throughout these discussions, references to the SG2524 apply also to the SG3524.
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
11POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
APPLICATION INFORMATION†
VIVO
VI > VO
VI
VI < VO
VO
VI–VO
| +VI | < | – VO |
Figure 10. Single-Ended Inductor Circuit
VO
Push-Pull
VO
VI
Flyback
ÏÏVI
Figure 11. Transformer-Coupled Outputs
† Throughout these discussions, references to the SG2524 apply also to the SG3524.
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
12 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
APPLICATION INFORMATION†
SG2524
COMP
.
CURR LIM+
EMIT 2
COL 2
COL 1
EMIT 1
GND
OSC OUT
CT
RT
REF OUT
IN+
IN–
0.01 µF
0.1 µF
5 kΩ
5 kΩ
2 kΩ
50 µF
–5 V20 mA
1N916
1N91620 µF
1N91615 kΩ
VCC = 15 V
VCC
CURR LIM–SHUTDOWN
+
1
2
16
6
7
10
3
11
12
13
14
4
5
9
8
15
5 kΩ
+
Figure 12. Capacitor-Diode Output Circuit
VCC = 5 V
0.1 µF1 MΩ
300 Ω
1N916
1N916
20T200 Ω
–15 V
20 mA
15 V
50 µF
50 µF
50T
50T
TIP29A
1 Ω
1N916620 Ω
510 Ω
2N2222
4.7 µF
0.001 µF
0.02 µF
5 kΩ
2 kΩ
100 µF
5 kΩ
5 kΩ
SG2524
VCC
OSC OUT
GNDCOMP
CURR LIM+
EMIT 2
COL 2
COL 1
EMIT 1
CURR LIM–
CT
RT
REF OUT
IN+
IN–
+
+
SHUTDOWN
25 kΩ
+
+
1
2
16
6
7
10
3
11
12
13
14
4
5
9
15
8
InputReturn
Figure 13. Flyback Converter Circuit
†Throughout these discussions, references to the SG2524 apply also to the SG3524.
SLVS077D – APRIL 1977 – REVISED FEBRUARY 2003
13POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
APPLICATION INFORMATION†
Input Return0.1 Ω
3 kΩ1N3880
500 µF
1 A5 V
0.9 mHTIP115
SG2524
VCC
OSC OUTGND
VCC = 28 V
0.001 µF
50 kΩ
5 kΩ
3 kΩ
0.1 µF
0.02 µF
5 kΩ
CURR LIM+
EMIT 2
COL 2
COL 1
EMIT 1
SHUTDOWN
CT
RT
REF OUT
IN+
IN–
CURR LIM–
COMP
1
2
16
6
7
10
3
11
12
13
14
4
5
9
15
8
5 kΩ
5 kΩ+
Figure 14. Single-Ended LC Circuit
5 kΩ
0.01 µF
0.1 µF
2 kΩ
5 kΩ
20 kΩ
1500 µF
0.1 Ω
100 µF
+
–5 A5 V
20T
20T
5T
5T
TIR101A
1 mH
TIP31A
100 Ω
100 Ω
TIP31A1W
1 kΩ
VCC = 28 V
GNDOSC OUT
VCC
SG2524
CURR LIM+
EMIT 2
COL 2
COL 1
EMIT 1
SHUTDOWN
CT
RT
REF OUT
IN+
IN–
CURR LIM–
COMP
1
2
16
6
7
10
3
11
12
13
14
4
5
9
15
8
5 kΩ
5 kΩ
0.001 µF
+
+
1W1 kΩ
Figure 15. Push-Pull Transformer-Coupled Circuit
†Throughout these discussions, references to the SG2524 apply also to the SG3524.
PACKAGING INFORMATION
Orderable Device Status (1) PackageType
PackageDrawing
Pins PackageQty
Eco Plan (2) Lead/Ball Finish MSL Peak Temp (3)
SG2524D ACTIVE SOIC D 16 40 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG2524DE4 ACTIVE SOIC D 16 40 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG2524DG4 ACTIVE SOIC D 16 40 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG2524DR ACTIVE SOIC D 16 2500 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG2524DRE4 ACTIVE SOIC D 16 2500 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG2524DRG4 ACTIVE SOIC D 16 2500 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG2524J OBSOLETE CDIP J 16 TBD Call TI Call TI
SG2524N ACTIVE PDIP N 16 25 Pb-Free(RoHS)
CU NIPDAU N / A for Pkg Type
SG2524NE4 ACTIVE PDIP N 16 25 Pb-Free(RoHS)
CU NIPDAU N / A for Pkg Type
SG3524D ACTIVE SOIC D 16 40 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524DE4 ACTIVE SOIC D 16 40 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524DG4 ACTIVE SOIC D 16 40 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524DR ACTIVE SOIC D 16 2500 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524DRE4 ACTIVE SOIC D 16 2500 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524DRG4 ACTIVE SOIC D 16 2500 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524J OBSOLETE CDIP J 16 TBD Call TI Call TI
SG3524N ACTIVE PDIP N 16 25 Pb-Free(RoHS)
CU NIPDAU N / A for Pkg Type
SG3524NE4 ACTIVE PDIP N 16 25 Pb-Free(RoHS)
CU NIPDAU N / A for Pkg Type
SG3524NS OBSOLETE SO NS 16 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524NSR ACTIVE SO NS 16 2000 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524NSRE4 ACTIVE SO NS 16 2000 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
SG3524NSRG4 ACTIVE SO NS 16 2000 Green (RoHS &no Sb/Br)
CU NIPDAU Level-1-260C-UNLIM
(1) The marketing status values are defined as follows:ACTIVE: Product device recommended for new designs.LIFEBUY: TI has announced that the device will be discontinued, and a lifetime-buy period is in effect.NRND: Not recommended for new designs. Device is in production to support existing customers, but TI does not recommend using this part ina new design.PREVIEW: Device has been announced but is not in production. Samples may or may not be available.OBSOLETE: TI has discontinued the production of the device.
PACKAGE OPTION ADDENDUM
www.ti.com 4-Jun-2007
Addendum-Page 1
Section 1. What are Ferrites?
Ferrites are dense, homogeneous ceramic structures made by mix-
ing iron oxide (Fe2O3) with oxides or carbonates of one or more
metals such as manganese, zinc, nickel, or magnesium. They are
pressed, then fired in a kiln at 2000°F, and machined as needed
to meet various operational requirements.
MAGNETICS ® Ferrites
Ferrites described in this catalog are the manganese-zinc type used
for communications (frequencies from 1KHz to 1000 KHz) and
for power applications such as in switching power supplies.
Advantages of Ferrites
Ferrites have a paramount advantage over other types of magnetic
materials: high electrical resistivity and resultant low eddy cur-
rent losses over a wide frequency range. Additional characteristics
such as high permeability and time/temperature stability have
expanded ferrite uses into quality filter circuits, high frequency
transformers, wide band transformers, adjustable inductors, delay
lines, and other high frequency electronic circuitry. As the high
frequency performance of other circuit components continues to
be improved, ferrites are routinely designed into magnetic circuits
for both low level and power applications. Another factor in choos-
ing ferrites is the higher cost of magnetic metals. For the most
favorable combination of low cost, high Q, high stability, and
lowest volume, ferrites are the best core material choice for fre-
quencies from 10 KHz to 50 MHz. Ferrites offer an unmatched
flexibility in magnetic and mechanical parameters.
Summary of Ferrite Advantages1. LOW COST
2. LARGE SELECTION OF MATERIALS
3. SHAPE VERSATILITY
4. ECONOMICAL ASSEMBLY
5. TEMPERATURE AND TIME STABILITY
6. HIGH RESISTIVITY
7. WIDE FREQUENCY RANGE (10 KHz to 50 MHz)
8. HIGH Q/SMALL PACKAGE
TYPICAL MECHANICAL AND THERMAL PROPERTIES OF FERRITE MATERIALSMechanical Data
Bulk DensityTensile Strength
Compressive Strength
Youngs Modulus
Hardness (Knoop)Resistivity
Thermal Data
Coef. of Linear ExpansionSpecific Heat (25°)
Thermal Conductivity (25-85°C)
4.855.07.0 x 10³4563 x 10³12.4 x 10³1 .8x107
650 Typical10²-10³
10.5 x 10- 6 °C - 1
1100 J.kg - 1 °C- 1
.26 cal.g - 1. °C- 1
3500-4300 µW.mm- 1. °C - 1
35-43 mW.cm - 1.°C- 1
.0083-.010 cal.s-¹.cm - 1 .°C - 1
Units
gm/cm³kgf.mm - 2
Ibs.in - 2
kgf.mm- 2
lbs.in - 2
kgf.mm - 2
Ibs.in- 2
ohm-cm
Units
Above properties are averages measured on a range of commercially availableMnZn ferrite materials.
1.1MAGNETIC • BUTLER, PA
Section 2. MaterialsMaterial Characteristics (1)
INDUCTORS AND LOWLEVEL APPLICATIONS
EMI/RFI FILTERS ANDBROADBAND TRANSFORMERS
MATERIALS A D G J W H
Initial Permeability µi — 750 ± 20% 2000 ± 20% 2300 ± 20% 5000 ± 20% 10000 ± 30% 15000 ± 30%
Maximum Usable Frequency(50% roll-off) f MHz <9 <4 <4 <1 <.25 <.15
tan δRelative Loss Factorµiac
10-6 <12 (.5MHz)<20 (1MHz)
<6 (.1MHz) <6 (.1MHz) <20(100kHz)
<7 (10kHz) <15 (10kHz)
*Curie Temperature Tc °C >260 >145 >180 >140 >125 >120
* Relative Temp. Factor- 30°C to +20°C+ 20°C to +70°C
/°C 10-6/°C2.0 to 4.0 (Typ.)
1.0 to 3.0.9 to 2.19 to 2.1 -. 7 to +.7
*Flux Density@ 1194 A/m (15 Oe)
Bm GmT
4600460
3800380
4600460
4300430
4300430
4200420
* Remanence Br GmT
2300230
1000100
1300130
1000100
80080
80080
* Coercivity Hc OeA/m
0.756
0.2520
0.1512
0.18
0.043
0.043
Disaccommodation Factor DF 10-6 <15 <2.0 <3.5 <3 <3 <2.5
* Resistivity ρ Ω-m 4 3 8 1 .15 .1
* Density δ g/cm3 4.5 4.7 4.7 4.8 4.8 4.9
*Power Loss (PL),
Sine Wave, in mW/cm²(typical)
25kHz200mT
(2000G)
@25°C@60°C@100°C@120°C
100kHz100mT(1000G)
@25°C@60°C@100°C@120°C
500kHz50mT(500G)
@25 °C@80°C
@100 °C@120 °C
225275
375
700kHz50mT(500G)
@25°C@60°C@100°C@120°C
Available in:
Pot Cores X X X X X
RS Cores X X X X
DS Cores X X
RM Cores X X X X X
EP Cores X X
E, U Cores X X
EC, ETD Cores
PQ Cores
Toroids X X X X X X
Blocks X
NOTE (1). These characteristics are typical for a 42206size (0.870" O.D.) toroid. Specific core data will usuallydiffer from these numbers due to the influence ofgeometry and size. Characteristics with * are typical.
2.1 MAGNETICS • BUTLER, PA
Material Characteristics (cont.) (1)
Br G 900m T 90
INDUCTORS ANDPOWER TRANSFORMERS
X
X
X
X
X
X
X
X
X
MATERIALS K R P F
Initial Permeability µj — 1500 ± 25% 2300 ± 25% 2500 ± 25% 3000 ± 20%
Maximum Usable Frequency(50% roll-off)
Relative Loss Factor
f MHz < 2 <1 .5 <1 .2 <1 .3
tan δ10-6µiac
Tc
/°C
<8(100kHz)
> 2 3 0 > 2 3 0 > 2 5 0° C >230* Curie Temperature
* Relative Temp. Factor–30°C to +20°C+20°C to +70°C
10- 6/°C
Bm G 4600mT 460
* Flux Density@ 1194 A/m (15 Oe)
* Remanence
5000 5000 4900
500 500 490
1100 1100 1200
110 110 120
0.18 0.18 0.214 14 16
* Coercivity Hc Oe 0.2A/m 16
Disaccommodation Factor 10 -6DF
p*Resisitivity Ω-m 20 6 5 2
δ 4.7 4.8 4.8 4.8*Density
*Power Loss (PL),Sine Wave, in mW/cm³(typical)
g/cm³
@25°C@60°C@100°C@120°C
25kHz
200mT
(2000G)
130 120 90
85 90 160
70 95 240
85 130
100kHz100mT
(1000G)
@25°C 100
@60°C 90@100°C 110
@120°C 130
125
90125
165
100180225
500kHz
50mT
(500G)
@25°C 100
@60°C 100
@100°C 120@120°C 140
300
250275
350
700kHz
50mT
(500G)
@25°C 180
@60°C 200@100°C 220@120°C 290
Available In:Pot Cores X X
X X
X X
X X
X X
X X
X X
X X
X X
X
RS Cores
DS Cores
X
X
X
X
X
X
X
X
X
X
RM Cores
EP Cores
E, U Cores
EC, ETD Cores
PQ Cores
Toroids
Blocks
MAGNETICS • BUTLER, PA 2.2
140
100
7090
375
300250
300
Graph 1 — Relative Loss Factor vs. Frequency Graph 2 — Initial Permeability (µi) vs. Temperature
Temperature °C
Frequency (kHz)
Graph 3A — Frequency Response Curves Graph 3B — Frequency Response Curves
Frequency (kHz)Frequency (kHz)
Graph 3C — Frequency Response Curves
Frequency (kHz)
2.3 MAGNETICS • BUTLER, PA
Saturation Flux Density - gausses 5000 ( at 15 oersted, 25° C) (500 mT)
Coercive Force - oersted . . . . . . . . 0.18 (14A/m)
Curie Temperature 230°C. . . . . . . . . . . . .
P Materialµ i
2500 ± 25%Note: The core loss curves are developed from empirical data. For bestresults and highest accuracy, use them. The formula on page 2.11 yields afair approximation and can be useful in computer programs.
CORE LOSS vs FLUX DENSITYPERMEABILITY vs. TEMPERATURE
TEMPERATURE (°C)
CORE LOSS vs. TEMPERATURE
TEMPERATURE (°C)
PERMEABILITY vs. FLUX DENSITYFLUX DENSITY GAUSS
FLUX DENSITY vs. TEMPERATURE
FLUX DENSITY GAUSS
See page 2.12 for B-H DataTEMPERATURE (°C)
2.6MAGNETIC • BUTLER, PA
CORE LOSS INFORMATION
Included on Pages 2.4-2.10 are material characteristics for the various Magnetics power and inductormaterials. For computer programming purposes, the core loss curves can be represented by theequation below. The factors indicated in the chart are split into discrete frequency ranges, so that theequation offers a close approximation to the core loss curves on the above pages.
CORE LOSS EQUATION: PL=af cBd
PL is in mW/cm3
B is in kGf is in kHz
FACTORS APPLIED TO THE ABOVE FORMULA
a c d
K Material f<500 kHz 0.0530 1.60 3.15
f>1 MHz 1.77*10-9 4.13 2.98
R Material f<100 kHz 0.074 1.43 2.85
100 kHz<f<500 kHz 0.036 1.64 2.68
f>500 kHz 0.014 1.84 2.28
P Material f<100 kHz 0.158 1.36 2.86
100kHz<f<500 kHz 0.0434 1.63 2.62
f>500 kHz 7.36*10-7 3.47 2.54
F Material f<10 kHz 0.790 1.06 2.85
10 kHz<f<100 kHz 0.0717 1.72 2.66
100 kHz<f<500 kHz 0.0573 1.66 2.68
f>500 kHz 0.0126 1.88 2.29
J Material f<20 kHz 0.245 1.39 2.50
f>20 kHz 0.00458 2.42 2.50
W Material f<20 kHz 0.300 1.26 2.60
f>20 kHz 0.00382 2.32 2.62
H Material f<20 kHz 0.148 1.50 2.25
f>20 kHz 0.135 1.62 2.15
2.11 MAGNETICS • BUTLER, PA
500 kHz<f<1 MHz 0.00113 2.19 3.10
B vs. H Curves (dc)
H-oersted H-oersted
H-oersted
H-oersted
H-oersted
CONVERSION TABLE
Multiplynumber ofOerstedsOerstedsGaussesGaussesTeslas
by to obtain
79.5 A/m.795 A/cm
.1 milli Teslas10 - 4 Teslas10 4 Gausses
2.12MAGNETICS • BUTLER, PA
Bibliography
[1] Muhammad H Rashid, Power Electronics Circuits, Devices and Applications,3rd
ed: Pearson Publication, 2004
[2] R S Anand Murthy and Nattarasu, Power electronics, 3rd ed:Pearson Publication
[3] L Umanand, S R Bhat, Design of Magnetic Components for Switched Mode Power
Converters
[4] Mohan, Ned, Tore M. Undeland, and William P. Robbins. Power Electronics. 3rd
ed. Hoboken: John Wiley & Sons, Inc., 2003.
[5] V Ramanarayanan, Power Switching Devices, Converters and Digital Simulation.
[6] SG3524 Data Sheet. www.ti.com/lit/ds/symlink/SG3524.pdf
59