1. ChapTer TwO DIODE APPLICATIONS
.…Electronic I.… ..DMT 121/3..
ChapTer TwO
DIODE APPLICATIONS

2. Load-Line Analysis
The analysis of electronic circuits can follow one of the two paths :
Practical characteristic or approximate model of the device.
Approximate model will be always used in the analysis
Approximate model

3. Load-Line Analysis
The load line plots all possible current (ID) conditions for all voltages applied to the diode (VD) in a given circuit. E / R is the maximum ID and E is the maximum VD.
Where the load line and the characteristic curve intersect is the Q-point, which specifies a particular ID and VD for a given circuit.
Fig Drawing the load line and finding the point of operation. 3

4. Slide (load line analysis)
The intersection of load line in Fig. 2.2 can
be determined by applying Kirchhoff’s
voltage in the clockwise direction, which
results in:
Fig Series diode configuration: (a) circuit.
Eq. (2.1)
ID and VD are the same for Eq. (2.1) and plotted load line in Fig. 2.2 (previous slide).
Set VD = 0 then we can get ID, where
Set ID = 0 then we get VD, where
Same with previous
Slide (load line analysis)

5. Example 2.1
For the series diode configuration of Fig. 2.3a, employing the diode characteristics of Fig. 2.3b, determine VDQ, IDQ and VR
Fig (a) Circuit; (b) characteristics.

6. Solution From the result, plot the straight line across ID and VD.
The resulting load line appears in Fig The Q points occurred at
VDQ  0.78 V IDQ  18.5mA
VR=IRR=IDQR=(18.5 mA)(1k) =18.5 V
Fig Solution to Example 2.1.  

7. Example 2.4
For the series diode configuration of Fig. 2.13, determine VD, VR and ID.
Solution:

8. Example 2.5 Repeat example 2.4 with the diode reversed Solution:
Open circuit

9. Introduction; Half – Wave Rectifier
The basic function of a DC power supply is to convert an AC voltage to a smooth DC voltage.
Fig. 2-1 Block Diagram of power supply

10. Sinusoidal Input : Half-Wave Rectification
Fig Half-wave rectifier.
Fig Nonconduction region (T/2  T).
Fig Conduction region (0  T/2).
Forward Bias
Reverse Bias

11. Average Value of Half-Wave Output Voltage
The average value of half-wave
rectified output voltage (also
called DC output voltage) is
The average value of the half-wave rectified output voltage (also known as DC voltage) is
31.8 % of Vm
The process of removing one-half the input signal to establish a dc level is called half-wave rectification
Fig Half-wave rectified signal.

12. Example: Half – Wave Rectifier
What is the average value of the half – wave rectified voltage?
50V
Vavg = 15.9 V

13. Effect of Barrier Potential (Silicon diode)
Fig Effect of VK on half-wave rectified signal.
Applied signal at least 0.7 for diode to turn on (Vk = 0.7V)
i ≤ 0.7 V  diode in open circuit and o = 0V
When conducting, Vk=0.7V ,then o= i – Vk  this cause reduction in o, thus reduce the resulting dc voltage level.
Now Vdc  (Vm – Vk)

14. Example: Effect of Barrier Potential
Draw the output voltages of each rectifier for the indicated input voltages.
Ans: Vout = 4.30 V
Ans: Vout = V

15. Peak Inverse Voltage (PIV)
Because the diode is only forward biased for one-half of the AC cycle, it is also reverse biased for one-half cycle.
It is important that the reverse breakdown voltage rating of the diode be high enough to withstand the peak, reverse-biasing AC voltage.
Peak inverse voltage is the maximum voltage across the diode when it is in reverse bias.
PIV = Vm OR accurately
PIV (or PRV)  Vm
PIV = Peak inverse voltage
PRV = Peak reverse voltage
Vm = Peak AC voltage
Diode must capable to withstand certain amount of repetitive reverse voltage

16. Full-Wave Rectifier
A full-wave rectifier allows current to flow during both the positive and negative half cycles or the full 360º. Note that the output frequency is twice the input frequency.
The average VDC or VAVG = 2Vp/.
Fig 2-11 Block Full Wave

17. Full-Wave Rectification
The rectification process can be improved by using more diodes in a full-wave rectifier circuit.
Full-wave rectification produces a greater DC output:
Full Wave Rectifier
Half-wave: Vdc = 0.318Vm = Vm/
Full-wave: Vdc = 0.636Vm = 2Vm/
Don’t confuse, some book use Vp; Vp = Vm
Half Wave Rectifier

18. Example: Full Wave rectified
Find the average value of the full-wave rectified voltage in Figure below.
Vavg = Vdc = 9.55 V

19. Full-Wave Rectification
Vo = Vi/2
Vo = Vi/2
Center-Tapped Transformer Rectifier
Requires
Two diodes
Center-tapped transformer
VDC = 0.636(Vm) 19

20. Full-Wave Center Tapped
Note the current flow direction during both alternations. Being that it is center tapped, the peak output is about half of the secondary windings total voltage.
Each diode is subjected to a PIV of the full secondary winding output minus one diode voltage drop.
PIV=2Vp(out) +0.7V
Fig 2-14 Center Tapped Current

21. Full-Wave Rectification
Bridge Rectifier
Four diodes are required
VDC = Vm

22. The Full-Wave Bridge Rectifier
The full-wave bridge rectifier takes advantage of the full output of the secondary winding.
It employs four diodes arranged such that current flows in the direction through the load during each half of the cycle.
Fig 2-20a&b

23. The Full-Wave Bridge Rectifier
The PIV for a bridge rectifier is approximately half the PIV for a center-tapped rectifier.
PIV=Vp(out) +0.7V
Fig 2-22b Full Wave w/diode drops
Note that in most cases we take the diode drop into account.

24. Summary of Rectifier Circuits
Ideal VDC
Practical (approximate) VDC
PIV
Half Wave Rectifier
VDC = 0.318(Vm)
= Vm/
VDC = 0.318(Vm – 0.7 )
PIV = Vm
Bridge Rectifier
VDC = 0.636(Vm)
= 2Vm/
VDC = 0.636(Vm) – 2(0.7))
PIV = Vm + 0.7V
Center-Tapped Transformer Rectifier
VDC = 0.318(Vm – 1.4)
PIV = 2Vm V
Vm = peak of the AC voltage. = Vp
In the center tapped transformer rectifier circuit, the peak AC voltage is the transformer secondary voltage to the tap. If used this, then
VDC = (Vm – 0.7)  do not confuse!!!!

25. Summary: Half-Wave Rectifier
Peak value of output:
Vp(out) = Vp(sec) – 0.7V
Average value of output
Diode peak inverse voltage
PIV = Vp(sec)

26. Summary: Center-Tapped Full-Wave Rectifier
Peak value of output:
Average value of output
Diode peak inverse voltage
PIV = 2Vp(sec) + 0.7V

27. Summary: Bridge Full-Wave Rectifier
Diode peak inverse voltage
PIV = Vp(sec) + 0.7V
Peak value of output:
Average value of output

28. Power Supply Filters And Regulators
In most power supply – 60 Hz ac power line voltage  constant dc voltage
Pulsating dc output must be filtered to reduce the large voltage variation
Small amount of fluctuation in the filter o/p voltage - ripple
ripple
Fig 2-24 Block Full Wave w/Filter

29. Power Supply Filters And Regulators (cont.) (Capacitor-Input Filter)
Fig 2-25a,b,&c

30. Capacitor Input Filter – Ripple Voltage
Ripple Voltage: the variation in the capacitor voltage due to charging and discharging is called ripple voltage
Ripple voltage is undesirable: thus, the smaller the ripple, the better the filtering action
The advantage of a full-wave rectifier over a half-wave is quite clear. The capacitor can more effectively reduce the ripple when the time between peaks is shorter. Figure (a) and (b)
Fig 2-28a&b
Easier to filter
-shorted time between
peaks.
-smaller ripple.

31. Capacitor-Input Filter – Ripple voltage
Ripple factor: indication of the effectiveness of the filter
(2-10)
[half-wave rectifier]
Vr(pp) = peak to peak ripple voltage; VDC = VAVG = average value of filter’s
output voltage.
Lower ripple factor  better filter
[can be lowered by increasing the value of filter capacitor
or increasing the load resistance]
(2-11)
For the full-wave rectifier:
Vp(rect) = unfiltered
peak.
(2-12)

32. Power Supply Filters And Regulators (cont.) (Capacitor-Input Filter)
Surge Current in the Capacitor-Input Filter:
Being that the capacitor appears as a short during the initial charging, the current through the diodes can momentarily be quite high. To reduce risk of damaging the diodes, a surge current limiting resistor is placed in series with the filter and load.
The min. surge
Resistor values:
Fig 2-31a&b
IFSM = forward surge
current rating
specified on
diode data sheet.
(2-13)

33. Power Supply Filters And Regulators
Regulation is the last step in eliminating the remaining ripple and maintaining the output voltage to a specific value. Typically this regulation is performed by an integrated circuit regulator. There are many different types used based on the voltage and current requirements.
Functions – maintains a constant output voltage (or current) despite changes in input, the load current, or the temperature.
Fig 2-33

34. Power Supply Filters And Regulators
How well the regulation is performed by a regulator is measured by it’s regulation percentage. There are two types of regulation, line and load. Line and load regulation percentage is simply a ratio of change in voltage (line) or current (load) stated as a percentage.
Line Regulation =
Load Regulation =

35. Diode Limiters (Clipper)
Clippers are networks that employ diodes to “clip” away of an input signal without distorting the remaining part of the applied waveform.

36. Diode Limiters (Clipper)

37. Example
What would you expect to see displayed on an oscilloscope connected across RL in the
limiter shown in above figure.

38. Solution
Assume approximate diode is used, Vd = 0.7 V

39. Biased Limiters (Clippers)
A positive limiter
The level to which an ac voltage is limited can be adjusted by adding a bias voltage, VBIAS in series with the diode
The voltage at point A must equal VBIAS V before the diode become forward-biased and conduct.
Once the diode begins to conduct, the voltage at point A is limited to VBIAS V, so that all input voltage above this level is clipped off.

40. Biased Limiters (Clippers)
A negative limiter
In this case, the voltage at point A must go below –VBIAS – 0.7V to forward-bias the diode and initiate limiting action as shown in the above figure.

41. Modified Biased Limiters (Clippers)

42. Example:
Figure above shows a circuit combining a positive limiter with a negative limiter. Determine the output voltage waveform ?

43. Solution :

44. Summary Limiters (Clippers)
In this examples VD = 0
In analysis, VD = 0 or VD = 0.7 V can be used. Both are right assumption.

45. Diode Clampers
A clamper is a network constructed of a diode, a resistor, and a capacitor that shifts a waveform to a different dc level without changing the appearance of the applied signal.
Sometimes known as dc restorers
Clamping networks have a capacitor connected directly from input to output with a resistive element in parallel with the output signal. The diode is also parallel with the output signal but may or may not have a series dc supply as an added elements.

46. Diode Clampers
FIGURE : Positive clamper operation. (Diode pointing up – away from ground)

47. Diode Clampers
FIGURE : Negative clamper operation (Diode pointing down – toward ground)

48. Diode Clamper
If diode is pointing up (away from ground), the circuit is a positive clamper.
If the diode is pointing down (toward ground), the circuit is a negative clamper

49. Diode Clamper (Square wave)
Diode ‘OF’ state
Output
Diode ‘ON’ state
V – Vc = 0 ; Vc = V; Vo = 0.7 V but ideal Vo = 0V
-V - Vc - Vo = 0; Vc = V
Vo = -2 V

50. Summary of Clamper Circuits

51. Voltage Multipliers
Voltage multiplier circuits use a combination of diodes and capacitors to step up the output voltage of rectifier circuits.
Voltage Doubler
Voltage Tripler
Voltage Quadrupler

52. Voltage Doubler
This half-wave voltage doubler’s output can be calculated by:
Vout = VC2 = 2Vm
where Vm = peak secondary voltage of the transformer 52

53. Voltage Doubler Positive Half-Cycle D1 conducts D2 is switched off
Capacitor C1 charges to Vm
Negative Half-Cycle
D1 is switched off
D2 conducts
Capacitor C2 charges to Vm
Vout = VC2 = 2Vm 53

54. Voltage Tripler and Quadrupler54

55. The Diode Data Sheet
The data sheet for diodes and other devices gives detailed information about specific characteristics such as the various maximum current and voltage ratings, temperature range, and voltage versus current curves (V-I characteristic).
It is sometimes a very valuable piece of information, even for a technician. There are cases when you might have to select a replacement diode when the type of diode needed may no longer be available.
These are the absolute max. values under which the diode can be operated without damage to the device.

56. The Diode Data Sheet (cont.) (Maximum Rating)
Symbol
1N4001
1N4002
1N4003
UNIT
Peak repetitive reverse voltage
Working peak reverse voltage
DC blocking voltage
VRRM
VRWM VR 50
100
200 V
Nonrepetitive peak reverse voltage
VRSM 60
120
240
rms reverse voltage
VR(rms) 35 70
140
Average rectified forward current (single-phase, resistive load, 60Hz, TA = 75oC Io 1 A
Nonrepetitive peak surge current (surge applied at rated load conditions)
IFSM
30 (for 1 cycle)
Operating and storage junction temperature range
Tj, Tstg
-65 to +175 oC

57. The Diode Data Sheet (cont.) (Maximum Rating)
FIGURE A selection of rectifier diodes based on maximum ratings of IO, IFSM, and IRRM.

58. Zener Diodes
The zener diode – silicon pn-junction device-designed for operate in the reverse-biased region
Zener diode symbol
Schematic diagram shown that this particular zener
circuit will work to maintain 10 V across the load

59. Zener Diodes
Breakdown voltage – set by controlling the doping level during manufacture
When diode reached reverse breakdown – voltage remains constant- current change
drastically
If zener diode is FB – operates the same as a rectifier diode
A zener diode is much like a normal diode – but if it is placed in the circuit in reverse
bias and operates in reverse breakdown.
Note that it’s forward characteristics are just like a normal diode.
1.8V – 200V

60. Zener Diodes
The reverse voltage (VR) is increased – the reverse current (IR) remains extremely
small up to the “knee”of the curve
Reverse current – called the zener current, IZ
At the bottom of the knee- the zener breakdown voltage (VZ) remains constant
although it increase slightly as the zener current, IZ increase.
IZK – min. current required to maintain voltage regulation
IZM – max. amount of current the diode can handle without being damage/destroyed
IZT – the current level at which the VZ rating of diode is measured (specified on a
data sheet)
The zener diode maintains a constant voltage for value of reverse current rating
from IZK to IZM

61. Zener Diodes (Zener Equivalent Circuit)
Since the actual voltage is not ideally vertical, the change in zener current
produces a small change in zener voltage
By ohm’s law:
Normaly -Zz is specified at IZT
(3-1)
Zener impedance

62. 3-1 Zener Diodes (cont.) (Temperature Coefficient & Zener Power Dissipation and Derating)
As with most devices, zener diodes have given characteristics such as
temperature coefficients and power ratings that have to be considered.
The data sheet provides this information (refer Figure 3-7).

63. Zener Diodes Applications
Zener diode can be used as
Voltage regulator for providing stable reference voltages
2. Simple limiters or clippers

64. Zener Regulation with Varying Input Voltage
As i/p voltage varies (within limits) – zener diode maintains a constant
o/p voltage
But as VIN changes, IZ will change, so i/p voltage variations are set
by the min. & max. current value (IZK & IZM) which the zener can
operate
Resistor, R –current limiting resistor

65. Zener Regulation with a Variable Load
The zener diode maintains a nearly constant voltage across RL as long as the zener current is greater than IZK and less than IZM
When the o/p terminal of the zener diode is open (RL=∞)-load current is zero and all of the current is through the zener
When a load resistor (R) is connected, current flow through zener & load RL, IL, IZ
The zener diode continues to regulate the voltage until IZ reaches its min value , IZK
At this point, the load current is max. , the total current through R remains
essentially constant.

66. Zener Limiting
Zener diode also can be used in ac applications to limit voltage swings to desired level
To limit the +ve peak of a signal voltage to the selected zener voltage
- During –ve alternation, zener arts as FB diode & limits the –ve voltage to -0.7V
b) Zener diode is turn around
-The –ve peak is by zener action & +ve voltage is limited to +0.7V
c) Two back-to-back zeners limit both peaks to the zener voltage ±7V
-During the +ve alternation, D2 is functioning as the zener limiter – D1 is functioning
as a FB diode.
-During the –ve alternation-the roles are reversed