zener diode as voltage regulator experiment result

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Lab # 007 - Best lab report

Electronic devices (ee-242), riphah international university.

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Lab title :-, zener regulation.

(a) To understand Zener regulation with a varying input voltage.

(b) To understand Zener regulation with a variable load.

(c) Zener as voltage clipper.

Objective :-

To study and verify the Voltage-Current relation in Zener Diodes by applying a voltage across it. Also observe Zener regulation by varying load resister. To study the diode applications in a clipping circuits. Understand the working of clipper circuit. Use a digital oscilloscope to capture and analyse output waveforms.

Introduction Of Theory:-

Zener diodes:.

Zener diode is a silicon semiconductor device that permits current to flow in either a forward or reverse direction. The diode consists of a special, heavily doped p-n junction, designed to conduct in the reverse direction when a certain specified voltage is reached..

An ideal P-N Junction diode does not conduct in reverse biased condition. A Zener diode Conducts excellently even in reverse biased condition. These diodes operate at a precise Value of voltage called break down voltage.

Zener Diode Clipping

Fig # 02 The Zener diode is acting like a biased diode clipping circuit with the bias voltage being equal to the Zener breakdown voltage. In this circuit during the positive half of the waveform the Zener diode is

reverse biased so the waveform is clipped at the Zener voltage, VZD1. During the negative half cycle the Zener acts like a normal diode with its usual 0 junction value.

Full-wave Zener Diode Clipping

The output waveform from full wave Zener diode clipping circuits resembles that of the previous voltage biased diode clipping circuit. The output waveform will be clipped at the Zener voltage plus the 0 forward volt drop of the other diode. So for example, the positive half cycle will be clipped at the sum of Zener diode, ZD1 plus 0 from ZD2 and vice versa for the negative half cycle.

Circuit Diagram :

Task # 1: varying input voltage effect on zener, task # 2: variable load effect on zener, task # 3: zener as voltage clipper.

Use Zener Diode = D2 = 3 Cut off Voltage Vin = 20 V

OUTPUT values from graph are:

Vpp = 11 Vmin = -4 Vmax = 7.

Tabular & Graphical Data :-

Using zener diode of 3v, sr. no. vin (v) vd (v), using zener diode of 12v , & 5kω variable resister, sr. no. vs (v) rl ( kω ) vl (v), discussion of results :-.

The zener diode act as the normal diode in the forward biased while increase in the value of the voltage the current at the certain level start increasing. The behaviour of the diode changes when the load resistance is changed But the main difference in the zener and the simple diode is in the reverse biased. The zener diode act as the voltage regulator The precautions are quite similar to that taken in a normal diode i  Excessive flow of current may damage the diode  Current for sufficiently long time may change the characteristics  Zener diodes are used in voltage regulation in circuits because even when,  A large current flows through, their voltage does not change appreciably.

Conclusion :-

This experiment is about to investigate the behavior of ZENER diode and analysis how it work. By observing the behavior of Zener diode on different applied voltages and find the results and calculation for its practical proves. Verify the Voltage-Current relation in Zener Diodes by applying a voltage across it. By changing resister value the voltage change at one limit, than no change in voltage. In this lab also understanding of clippers that what are clippers circuits how and why they are formed and how to use diodes to make clipper circuits. Moreover, to analyse the working of diode in limiters or clippers and to find the waveforms. At the end, all the required values and circuits are obtained with the help of oscilloscope.

References :-

 electric-shocks/forward-and-reverse-bias-of-di ode-explained-by-v-i-characteristic- curves/  electronics-tutorials/blog/i-v-characteristic- curves  quora/What-is-the-cut-in-voltage-of-a-diode

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University : riphah international university.

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The Zener Diode

A Semiconductor Diode blocks current in the reverse direction, but will suffer from premature breakdown or damage if the reverse voltage applied across becomes too high

However, the Zener Diode or “Breakdown Diode”, as they are sometimes referred too, are basically the same as the standard PN junction diode exept that they are specially designed to have a low and specified Reverse Breakdown Voltage which takes advantage of any reverse voltage applied to it.

In the forward-biased direction, that is Anode is more positive with respect to its Cathode, a zener diode behaves like a normal junction diode when the forward voltage V F across the diode exceeds 0.7 volts (silicon) causing the zener diode to conduct.

The forward current flowing through the conducting diode is at its maximum determined only by the connected load. Thus in the forward-bias direction, the zener behaves like a regular diode within its specified current and/or power limits and as such, the forward characteristics of a zener diode is generally of no interest.

However, unlike a conventional diode that blocks any flow of current through itself when reverse biased, that is the Cathode becomes more positive than the Anode, as soon as the reverse voltage reaches a pre-determined value, the zener diode begins to conduct in the reverse direction.

Since a zener diode is designed to work in the reverse breakdown region of its characteristic curve, they have a fixed breakdown voltage, V Z value which is determined during manufacture. As the reverse voltage across the zener diode increases from 0 volts to its zener breakdown voltage, a small reverse or leakage current will flow through the diode which remains fairly constant as the reverse voltage increases.

Once the reverse voltage applied across the zener diode exceeds the rated voltage of the device, a process called Zener Breakdown occurs in the semiconductor depletion layer and a current starts to flow through the diode to limit this increase in voltage.

The current now flowing through the zener diode increases dramatically to its maximum circuit value (which is usually limited by a series resistor). Once zener breakdown occurs, the voltage drop across the diode remains fairly constant even though the zener current, I Z through it can vary considerably. The voltage point at which the voltage across the zener diode becomes stable is called the “zener voltage”, ( V Z ). For zener diodes this breakdown voltage value can range from a few volts upto a few hundred volts.

The point at which the zener voltage triggers the current to flow through the diode can be very accurately controlled (to less than 1% tolerance) in the doping stage of the diodes semiconductor construction giving the diode a specific zener breakdown voltage , (  V Z  ) for example, 4.3V or 7.5V. This zener breakdown voltage on the I-V curve is almost a vertical straight line.

Zener Diode I-V Characteristics

The Zener Diode is used in its “reverse bias” or reverse breakdown mode, i.e. the diodes anode connects to the negative supply. From the I-V characteristics curve above, we can see that the zener diode has a region in its reverse bias characteristics of almost a constant negative voltage regardless of the value of the current flowing through the diode.

This voltage remains almost constant even with large changes in current providing the zener diodes current remains between the breakdown current I Z(min) and its maximum current rating I Z(max) .

This ability of the zener diode to control itself can be used to great effect to regulate or stabilise a voltage source against supply or load variations. The fact that the voltage across the diode in the breakdown region is almost constant turns out to be an important characteristic of the zener diode as it can be used in the simplest types of voltage regulator applications.

The function of a voltage regulator is to provide a constant output voltage to a load connected in parallel with it in spite of the ripples in the supply voltage or variations in the load current. A zener diode will continue to regulate its voltage until the diodes holding current falls below the minimum I Z(min) value in the reverse breakdown region.

The Zener Diode Regulator

Zener Diodes can be used to produce a stabilised voltage output with low ripple under varying load current conditions. By passing a small current through the diode from a voltage source, via a suitable current limiting resistor ( R S ), the zener diode will conduct sufficient current to maintain a voltage drop of Vout .

We remember from the previous tutorials that the DC output voltage from the half or full-wave rectifiers contains ripple superimposed onto the DC voltage and that as the load value changes so to does the average output voltage. By connecting a simple zener stabiliser circuit as shown below across the output of the rectifier, a more stable output voltage can be produced.

Zener Diode Regulator

Resistor, R S is connected in series with the zener diode to limit the current flow through the diode with the voltage source, V S being connected across the combination. The stabilised output voltage V out is taken from across the zener diode.

The zener diode is connected with its cathode terminal connected to the positive rail of the DC supply so it is reverse biased and will be operating in its breakdown condition. Resistor R S is selected so to limit the maximum current flowing in the circuit.

With no load connected to the circuit, the load current will be zero, (  I L  = 0  ), and all the circuit current passes through the zener diode which in turn dissipates its maximum power.

Also a small value of the series resistor R S will result in a greater diode current when the load resistance R L is connected and large as this will increase the power dissipation requirement of the diode so care must be taken when selecting the appropriate value of series resistance so that the zener’s maximum power rating is not exceeded under this no-load or high-impedance condition.

The load is connected in parallel with the zener diode, so the voltage across R L is always the same as the zener voltage, (  V R  = V Z  ).

There is a minimum zener current for which the stabilisation of the voltage is effective and the zener current must stay above this value operating under load within its breakdown region at all times. The upper limit of current is of course dependant upon the power rating of the device. The supply voltage V S must be greater than V Z .

One small problem with zener diode stabiliser circuits is that the diode can sometimes generate electrical noise on top of the DC supply as it tries to stabilise the voltage. Normally this is not a problem for most applications but the addition of a large value decoupling capacitor across the zener’s output may be required to give additional smoothing.

Then to summarise a little. A zener diode is always operated in its reverse biased condition. As such a simple voltage regulator circuit can be designed using a zener diode to maintain a constant DC output voltage across the load in spite of variations in the input voltage or changes in the load current.

The zener voltage regulator consists of a current limiting resistor R S connected in series with the input voltage V S with the zener diode connected in parallel with the load R L in this reverse biased condition. The stabilised output voltage is always selected to be the same as the breakdown voltage V Z of the diode.

Tutorial Example No1

A 5.0V stabilised power supply is required to be produced from a 12V DC power supply input source. The maximum power rating P Z of the zener diode is 2W. Using the zener regulator circuit above calculate:

a).  The maximum current flowing through the zener diode.

b).  The minimum value of the series resistor, R S

c).  The load current I L if a load resistor of 1kΩ is connected across the zener diode.

d).  The zener current I Z at full load.

Zener Diode Voltages

As well as producing a single stabilised voltage output, zener diodes can also be connected together in series along with normal silicon signal diodes to produce a variety of different reference voltage output values as shown below.

Zener Diodes Connected in Series

The values of the individual Zener diodes can be chosen to suit the application while the silicon diode will always drop about 0.6 – 0.7V in the forward bias condition. The supply voltage, Vin must of course be higher than the largest output reference voltage and in our example above this is 19v.

A typical zener diode for general electronic circuits is the 500mW, BZX55 series or the larger 1.3W, BZX85 series were the zener voltage is given as, for example, C7V5 for a 7.5V diode giving a diode reference number of BZX55C7V5 .

The 500mW series of zener diodes are available from about 2.4 up to about 100 volts and typically have the same sequence of values as used for the 5% (E24) resistor series with the individual voltage ratings for these small but very useful diodes are given in the table below.

Zener Diode Standard Zener Voltages

Zener clipping circuits.

Thus far we have looked at how a zener diode can be used to regulate a constant DC source but what if the input signal was not steady state DC but an alternating AC waveform how would the zener diode react to a constantly changing signal.

Diode clipping and clamping circuits are circuits that are used to shape or modify an input AC waveform (or any sinusoid) producing a differently shape output waveform depending on the circuit arrangement. Diode clipper circuits are also called limiters because they limit or clip-off the positive (or negative) part of an input AC signal. As zener clipper circuits limit or cut-off part of the waveform across them, they are mainly used for circuit protection or in waveform shaping circuits.

For example, if we wanted to clip an output waveform at +7.5V, we would use a 7.5V zener. If the output waveform tries to exceed the 7.5V limit, the diode will “clip-off” the excess voltage from the input producing a waveform with a flat top still keeping the output constant at +7.5V.

Note that in the forward bias condition a zener diode is still a diode and when the AC waveform output goes negative below -0.7V, the zener diode turns “ON” like any normal silicon diode would and clips the output at -0.7V as shown below.

Square Wave Signal

The back to back connected zener diodes can be used as an AC regulator producing what is jokingly called a “poor man’s square wave generator”. Using this arrangement we can clip the waveform between a positive value of +8.2V and a negative value of -8.2V for a 7.5V zener diode.

So for example, if we wanted to clip an output waveform between two different minimum and maximum values of say, +8V and -6V, we would simply use two differently rated zener diodes. Note that the output will actually clip the AC waveform between +8.7V and -6.7V due to the addition of the forward biasing diode voltage.

In other words a peak-to-peak voltage of 15.4 volts instead of expected 14 volts, as the forward bias volt drop across the diode adds another 0.7 volts in each direction.

This type of clipper configuration is fairly common for protecting an electronic circuit from over voltage. The two zener’s are generally placed across the power supply input terminals and during normal operation, one of the zener diodes is “OFF” and the diodes have little or no affect. However, if the input voltage waveform exceeds its limit, then the zener’s turn “ON” and clip the input to protect the circuit.

In the next tutorial about diodes , we will look at using the forward biased PN junction of a diode to produce light. We know from the previous tutorials that when charge carriers move across the junction, electrons combine with holes and energy is lost in the form of heat, but also some of this energy is dissipated as photons but we can not see them.

If we place a translucent lens around the junction, visible light will be produced and the diode becomes a light source. This effect produces another type of diode known commonly as the Light Emitting Diode which takes advantage of this light producing characteristic to emit light (photons) in a variety of colours and wavelengths.

Read more Tutorials inDiodes

• 1. Semiconductor Basics
• 2. PN Junction Theory
• 3. PN Junction Diode
• 4. The Signal Diode
• 5. Power Diodes and Rectifiers
• 6. Full Wave Rectifier
• 7. The Zener Diode
• 8. The Light Emitting Diode
• 9. Bypass Diodes in Solar Panels
• 10. Diode Clipping Circuits
• 11. The Schottky Diode

376 Comments

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I WANT TO DROP 48VC TO 14VDC AND HÀVE 25 AMPS

Calculation please

Good information

Perfect catch quick revision. Thanks

Your content is very benefical to every students.

Zener diode as voltage regulator

I am student.It is very useful for me and also support in my lesson.

Ignation problem about zoomerx there a current but cannot start the engine

which zener diode can I use to replace 33v 1watt zener diode

33V, 1 watt or greater

I can replace 33v1watt zener diode with 15volts1watt zener diode. can it wok with out problems

I love this

How to use zener diode with ptc thermister

I learn electronic

I have an output of 55vdc i need to power an led display (volt meter) I can use a 12volt or a 24volt zener diode they are 5 watts which i believe are a lot more than i need. what size resistor would i use for this ? can i do this with one resistor and one diode? thanks Vic

The resistive value of your series resistor would depend on the load current required by the led display. A 24V, 5W zener requires a maximum zener current of 200mA (5/24), while the 12V, 5W zener requires 400mA (5/12). Then R S = (55 – V Z )/(I Z + I LED ). P R = I 2 *R s

Suburb tutorial right to the point

This will helpwith my experiments and designs, thank you.

I want to use a zener diode of 4V3 with a small solar panel and looking at about 200mA. The panel will either be 5V / 5V5 /6V. When it is starting, it will have lower voltage, so, using a zener, will the voltage still go thru if it is under 4V or will it only work once the voltage is 5V and reduce it to 4V3?

A small boost circuit that will boost it to 5V will be used, but it has a tolerance of 0V8 – 5V and would like to be harvesting from low voltages.

Sir Z Zzenar diode and Zzenar what’s diffrent between

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 Controls

Insert Key Button : This is used to insert key on the switch connected with battery. This key is only activated when the connection is perfect.

Choose Zener Diode: This combo box is used to select different zener diodes having different zener voltage

Series Resistance :  Value of the Series Resistance can be directly input here.

Rheostat value:  Rheostat can be controlled by using this slider

Load Resistance:  Value of load resistance can be set or change by using this slider

Reset Button:  To reset all the connections

 Procedure

Using the circuit diagram, identify the connections in the given platform. Connections are made as shown in the below diagram.

How to make connections in simulation ?

Click one end node of the battery and drag to the next position, where we want to connect the wire. Just like shown in the figures below:

                                            (a)                                                         (b)                                                      (c) 

 Like this, make all the connections are perfect.

Full connection diagram 

 If the connections are correct, Insert Key option activated

Line regulation

• Choose the zener diode to start the experiment.
• Insert the series resistance value.
• Fix the load resistance value by using Load Resistance slider.
• Change the Rheostat value from maximum to 0 by the interval 100.
• Note down the corresponding input voltage and output voltage and tabulate it.
• Plot the graph in which V IN at x-axis V L at y-axis.

 Load Regulation

• First 3 steps are same as above.
• Fix the Rheostat value, to get the 12 V at voltmeter across rheostat. 
• Change the load Resistance with the interval of 100 Ω/1000 Ω up to maximum range.
• Note  the reading and tabulate it.
• Plot the graph between V 0 along x-axis and R L along y-axis.

Let us consider V NL  is the output voltage when there is no load resistance (ideally V NL = Zener voltage) and V FL  is the output voltage when load resistance is maximum. 

Note:  This is an ideal circuit. For a real circuit, there will be small variations in output voltage with varying input voltage or load resistance.

Cite this Simulator: