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EC2155-Circuits and Devices lab

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    VERIFICATION OF KIRCHHOFFS CURRENT LAW

    CIRCUIT DIAGRAM

    TABULATION:

    S.no Supply Voltage (V) I1 (mA) I2 (mA) I3 (mA)I2 + I3

    (mA)

    1

    2

    3

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    Expt.No:1

    Verification of KCL and KVL

    Aim:

    To verify a) Kirchhoffs Current Law

    b) Kirchhoffs Voltage Law

    Materials Required:

    S.No Components/Equipments Range Quantity

    1 RPS (0-15)V 1

    2 Ammeter (0-30)mA 3

    3 Voltmeter (0-30)V 2

    4 Resistors 5001K

    3.3K

    11

    2

    5 Bread Board 16 Connecting Wires As reqd.

    Theory:

    Kirchhoffs Current Law (KCL)

    Kirchhoffs Current Law states that the algebraic sum of all currents at any node in a

    circuit is zero.

    i.e. sum of currents entering a node = sum of currents leaving the node

    Procedure:

    Kirchhoffs Current Law (KCL)

    1. Make connections as per the circuit diagram.2. Switch on the power supply.3. Note down the ammeter readings and verify KCL.4. Repeat the experiment with different values of supply voltages.

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    VERIFICATION OF KIRCHHOFFS VOLTAGE LAW

    CIRCUIT DIAGRAM

    TABULATION:

    S.no Supply Voltage (V) V1 (V) V2 (V) V3 (V) V1 + V2 + V3

    1

    2

    3

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    Theory:

    Kirchhoffs Voltage Law (KVL)

    Kirchhoffs Voltage Law states that the algebraic sum of all voltages across any set of

    branches in a closed loop is zero.

    i.e. sum of voltage drop = sum of voltage rise

    Procedure:

    Kirchhoffs Voltage Law (KVL)

    1. Make connections as per the circuit diagram.2. Switch on the power supply.3. Note down the voltmeter readings and verify KVL.4. Repeat the experiment with different values of supply voltages.

    Result:

    Thus Kirchhoffs Current and Voltage laws were verified.

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    VERIFICATION OF THEVENINS THEOREM

    CIRCUIT DIAGRAM

    Figure 1:

    Figure 2:

    Figure 3:

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    Expt.No:2

    Verification of Thevenin and Nortons Theorem

    Aim:

    To verify a) Thevenins Theorem

    b) Nortons Theorem

    Materials Required:

    S.No Components/Equipments Range Quantity

    1 RPS (0-30)V 1

    2 Ammeter (0-1)mA 1

    3 Voltmeter (0-10)V 1

    4 DRB (0-1)M 1

    5 Resistors 560

    1K470

    10K5.6K

    1

    21

    32

    6 Bread Board 1

    7 Connecting Wires As reqd.

    Theory:

    Thevenins Theorem

    Thevenins theorem states that any two-terminal linear network having a number of

    voltage, current sources and resistances can be replaced by a simple equivalent circuit consisting

    of a single voltage source in series with a resistance, where the value of the voltage source is

    equal to the open circuit voltage across the two terminals of the network and resistance is equalto the equivalent resistance measured between the terminals with all the energy sources replaced

    by their internal resistances.

    Procedure:

    Thevenins Theorem

    1. Connect the circuit as shown in the circuit diagram.2. Measure the voltage across the load (VL) using a voltmeter or multimeter after switching

    on the power supply.

    To find Thevenins Equivalent Circuit:

    3. Remove the load resistance and measure the open circuited voltage VTH across the outputterminal (as in figure 2).

    4. Remove the voltage source and measure the resistance RTH across the output (as in figure3) using multimeter.

    5. Connect the Thevenin equivalent circuit as in figure 4.6. Measure the value of load voltage VL across the load resistance.

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    Figure 4:

    THEVENINS EQUIVALENT CIRCUIT

    TABULATION:

    S.No VS RL VL RTH VTH VL

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    VERIFICATION OF NORTONS THEOREM

    CIRCUIT DIAGRAM

    Figure 5:

    Figure 6:

    Figure 7:

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    Theory:

    Nortons Theorem

    Nortons theorem states that any two-terminal linear network with current sources,

    voltage sources and resistances can be replaced by a simple equivalent circuit consisting of a

    current source in parallel with a resistance. The value of the current source is the short circuit

    current between the two terminals of the network and the resistance is the equivalent resistance

    measured between the terminals of the network with all the energy sources replaced by their

    internal resistances.

    Procedure:

    Nortons Theorem

    1. Connect the components as shown in the given circuit. (Figure 5).2. Measure the current through the load IL using an ammeter or multimeter.

    To find Nortons equivalent circuit:3. Remove the load resistance and short circuit the output terminal. Measure the current IN

    through the short circuited terminals.

    4. Remove the voltage source and measure the resistance across the output terminal.5. Connect the components as in the equivalent circuit where Veq = IN . RN volt.6. Measure the load current IL through the load resistorRL.7. Verify if IL = IL.

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    Figure 8:

    Figure 9:

    NORTONS EQUIVALENT CIRCUIT

    TABULATION:

    S.NoVS(V)

    IL

    (mA)

    IN

    (mA)

    RN

    (K)Veq = IN.RN

    (V)

    IL(mA)

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    Result:

    Thus Thevenins and Nortons theorems were verified.

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    VERIFICATION OF SUPERPOSITION THEOREM

    CIRCUIT DIAGRAM

    Figure 1:

    Figure 2:

    Figure 3:

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    Expt.No:3

    VERIFICATION OF SUPERPOSITION THEOREM

    Aim:

    To verify Superposition theorem.

    Components Required:

    S.No Components/Equipments Range Quantity

    1 RPS (0-30)V 1

    2 Ammeter (0-50)mA 1

    3 DRB (0-1)M 1

    4 Resistors 330

    470

    1

    1

    5 Bread Board 1

    6 Connecting Wires As reqd.

    Theory:Superposition Theorem

    It states that in any linear resistive network, the voltage across or current through any

    resistor or source may be calculated by adding algebraically all the individual voltages or

    currents caused by separate independent sources acting alone, with all the other independent

    voltage sources replaced by short circuits and all other independent current sources replaced by

    open circuits. However, superposition theorem is not applicable to unbalanced bridge circuits.

    The theorem is applicable only to linear circuits. The theorem cannot be used to measure power

    and it is applicable only for circuits having more than one source.

    Procedure:

    1. Connect the circuit as in the given circuit (Figure1).2. Switch on the power supply.3. Adjust the DRB to a certain value and measure the ammeter reading, I.4. Set V2 to a certain value and short circuit the voltage source V1 as in Figure 2, and

    measure the ammeter reading, I1.

    5. Set V1 at a certain value and short circuit the second voltage source V2 (as in Figure 3).Measure the ammeter reading, I2.

    6. Verify if I = I1 + I2.7.

    Repeat the experiment for different DRB values.

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    TABULATION:

    S.No

    DRB

    value

    ()

    I

    (mA)

    I1

    (mA)

    I2

    (mA)I1 + I2(mA)

    Theoretical Practical Theoretical Practical Theoretical Practical

    1

    2

    3

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    Result:

    Thus Superposition theorem was verified.

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    VERIFICATION OF MAXIMUM POWER TRANSFER THEOREM

    CIRCUIT DIAGRAM:

    TABULATION:

    S.No DRB Value, R

    ()Current, I

    (mA)

    Power, P= I2R

    (W)

    1.

    2.

    3.

    4.

    5.

    MODEL GRAPH:

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    Expt.No:4

    VERIFICATION OF MAXIMUM POWER TRANSFER & RECIPROCITY THEOREMS

    Aim:

    To verify Maximum Power transfer and Reciprocity theorems.

    Components Required:

    S.No Components/Equipments Range Quantity

    1 RPS (0-10)V 1

    2 Ammeter (0-30)mA 1

    3 DRB (0-1)M 1

    4 Resistors 3.3K

    2.2K1K

    1

    11

    5 Bread Board 1

    6 Connecting Wires As reqd.

    Maximum Power Transfer Theorem

    Theory:

    Maximum Power Transfer theorem states An independent voltage source in series with a

    resistance RS, delivers a maximum power to that loads resistance RL for which RL = RS .

    Maximum Power Transfer theorem can also be stated in terms of Thevenin equivalent

    resistance of the network as A network delivers the maximum power to a load resistance RL

    when RLis equal to the Thevenin equivalent resistance of the network.

    Procedure:

    1. Connect the circuit as shown in figure.2. Find the Thevenin equivalent resistance of the circuit.3. Adjust the DRB for different values of resistances and note down the ammeter readings.4. Calculate the power for the corresponding resistance and current readings.5. Verify if power is maximum for RL = RTH.

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    VERIFICATION OF RECIPROCITY THEOREM

    CIRCUIT DIAGRAM

    Figure 1:

    Figure 2:

    TABULATION:

    S.NoVoltage, V1

    (V)

    Current I1

    (mA)V1 / I1

    Voltage, V2

    (V)

    Current I2

    (mA)V2 / I2

    1.

    2.

    3.

    4.

    5.

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    Reciprocity Theorem

    Theory:

    Reciprocity theorem states In any passive linear bilateral network, if the single voltage

    source Vx in the branch x produces the current response Iy in the branch y, then the removal of

    the voltage source from the branch x and its insertion in the branch y will produce the current

    response Iy in the branch x.

    In other words, In a linear network, if the position of the excitation and response are

    interchanged, their ratio remains the same.

    Procedure:

    1. Connect the circuit as in figure 1.2. For different values of V1, note down the corresponding values of I1 in the ammeter.3. Calculate the values of V1/I1 and tabulate them.4. Now change the circuit as in figure 2.5.

    For different values of V2, note down the corresponding values of I2 in the ammeter.

    6. Calculate the values of V2/I2 and tabulate them.7. Verify if V1/I1 = V2/I2.

    Result:

    Thus Maximum power transfer theorem and reciprocity theorems were verified.

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    SERIES RESONANCE CIRCUIT

    CIRCUIT DIAGRAM:

    TABULATION:

    S.NoInput Frequency

    (Hz)

    Output Voltage

    (V)

    MODEL GRAPH:

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    Expt.No:5

    FREQUENCY RESPONSE OF SERIES AND PARALLEL RESONANCE CIRCUITS

    Aim:

    To find the resonant frequency of series and parallel RLC circuits.

    Components Required:

    S.No Components/Equipments Range Quantity

    1 Function Generator (0-1)MHz 1

    2 Voltmeter (0-5)V 1

    3 Resistor 1K 1

    4 Capacitor 1F 1

    5 Inductor 50mH 1

    6 Bread Board 1

    7 Connecting Wires As Reqd.,

    Theory:The resonance of a series RLC circuit occurs when the inductive and capacitive reactance

    are equal in magnitude but cancel each other because they are 180 apart in phase. It has

    minimum impedance at resonance frequency and the phase angle at resonance is equal to zero.

    In parallel RLC circuits the circuit behaves purely resistive at resonance. Since inductive

    and capacitive reactance currents are equal and opposite in phase, they cancel one another at

    parallel resonance. If a capacitor and an inductor, each with negligible resistance are connected

    in parallel and the frequency is adjusted such that the reactances are exactly equal, current will

    flow through the inductor and capacitor, but the total current will be negligible. The impedance

    of parallel RLC circuit is almost infinite.

    Formula Used:

    Resonant frequency, fr=

    (Hz)

    Procedure:

    1. The connections are made as per the circuit diagram.2. Vary the input frequency and tabulate the corresponding voltage readings.3. Plot the graph and note down the resonant frequency from the graph.4. Verify if the resonant frequency from the graph is equal to the theoretical resonant

    frequency.

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    PARALLEL RESONANCE CIRCUIT

    CIRCUIT DIAGRAM

    TABULATION:

    S.NoInput Frequency

    (Hz)

    Output Voltage

    (V)

    MODEL GRAPH:

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    Result:

    Thus series and parallel resonant circuits were constructed and their frequency response

    curves were drawn.

    Resonant frequency of series RLC circuit =

    Resonant frequency of parallel RLC circuit =

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    CHARACTERISTICS OF PN-JUNCTION DIODE

    CIRCUIT DIAGRAM:

    FORWARD BIAS:

    REVERSE BIAS:

    CIRCUIT SYMBOL:

    MODEL GRAPH

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    Expt.No:6

    CHARACTERISTICS OF P-N JUNCTION DIODE AND ZENER DIODE

    Aim:

    To plot the V-I characteristics of the given PN junction diode and Zener diode under

    forward bias and reverse bias.

    Components Required:

    S.No Components/Equipments Range Quantity

    1 PN junction diode 1N4001 1

    2 Zener diode 1

    3 Ammeter (0-50)mA

    (0-500)A

    1

    1

    4 Voltmeter (0-1)V

    (0-30)V

    1

    1

    5 Resistor 1K 16 RPS (0-15)V 1

    7 Connecting Wires As Reqd.,

    PN Junction Diode

    Theory:

    If donor impurities are introduced into one side and acceptor into the other side of a

    single crystal of a semiconductor, a p-n junction is formed. Initially there are only p-type carriers

    to the left of the junction and only n-type carriers to the right of the junction.

    Forward Bias:

    The P-type of the semiconductor is connected to the positive of the battery and N-type tothe negative of the battery.

    Width of the depletion region decreases with increase in the bias voltage. Hence there is gradual increase in current with increasing voltage.

    Reverse Bias:

    The P-type of the semiconductor is connected to the negative of the battery and N-type tothe positive of the battery.

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    P-N JUNCTION DIODE

    TABULATION:

    FORWARD BIAS:

    S.No Forward Voltage

    VF (V)

    Forward Current

    IF (V)

    REVERSE BIAS:

    S.No Reverse Voltage

    VR(V)

    Reverse Current

    IR(V)

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    Width of the depletion region increases with increase in bias voltage which results in highresistance.

    Hence minimum current flows through the diode.Formula Used:

    Resistance = V / I (ohms)

    Procedure:

    1. Make connections as per the circuit diagram.2. Vary the voltage in the regulated power supply and note down the corresponding

    ammeter and voltmeter readings.

    3. Tabulate the readings and plot the graph with voltage in X-axis and current in Y-axis.4. Calculate the value of forward resistance.

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    CHARACTERISTICS OF ZENER DIODE

    CIRCUIT DIAGRAM:

    FORWARD BIAS:

    REVERSE BIAS:

    CIRCUIT SYMBOL:

    V-I CHARACTERISTICS:

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    ZENER DIODE

    Theory:

    The zener diode uses a p-n junction in reverse bias to make use of the zener effect

    (breakdown phenomenon) which holds the voltage close to a constant value called the zener

    voltage. The constant reverse voltage VZ of the zener diode makes it a valuable component for

    the regulation of the output voltage against both variations in the input voltage from an

    unregulated power supply or variations in the load resistance.

    Procedure:

    1. Make connections as per the circuit diagram.2. Vary the voltage in the regulated power supply and note down the corresponding

    ammeter and voltmeter readings.

    3. Tabulate the readings and plot the graph with voltage in X-axis and current in Y-axis.4. Note down the value of zener voltage VZ.

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    ZENER DIODE

    TABULATION:

    FORWARD BIAS:

    S.No Forward Voltage

    VF (V)

    Forward Current

    IF (V)

    REVERSE BIAS:

    S.No Reverse Voltage

    VR(V)

    Reverse Current

    IR(V)

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    CHARACTERISTICS OF CE CONFIGURATION

    CIRCUIT DIAGRAM:

    INPUT CHARACTERISTICS:

    OUTPUT CHARACTERISTICS:

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    Expt.No:7

    CHARACTERISTICS OF CE CONFIGURATION

    Aim:

    To plot the input and output characteristics of a given BJT in CE configuration and

    determine its hybrid parameters.

    Components Required:

    S.No Components/Equipments Range Quantity

    1 Bipolar Junction Transistor BC 107 1

    2 Ammeter (0-10)mA

    (0-500)A

    1

    1

    3 Voltmeter (0-5)V

    (0-10)V

    1

    1

    4 Resistor 10K 1

    5 RPS (0-15)V 26 Connecting Wires As Reqd.,

    Theory:

    In CE configuration, the base is taken as input terminal, collector is taken as output

    terminal and emitter is taken as common terminal. The input characteristics are drawn for

    different values of IB and VBE with VCE constant. The output characteristics are drawn for

    different values of IC and VCE with IB constant.

    Procedure:

    1. Make connections as per the circuit diagram.2. To obtain the input characteristics, keep the value of VCE constant. For different values of

    VBE, tabulate the corresponding values of IB.

    3. Repeat the procedure for various constant values of VCE.4. Plot the graph and calculate the hybrid parameters.5. To obtain the output characteristics, keep the value of IB constant. For different values of

    VCE, tabulate the corresponding values of IC.

    6. Repeat the procedure for various constant values of IB.7. Plot the graph and calculate the hybrid parameters.

    Formula Used:

    1. Input Impedance (hie) =

    , VCE = constant

    2. Forward Current Gain (hfe) =

    , VCE = constant

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    PIN DIAGRAM SYMBOL

    TABULATION:

    INPUT CHARACTERISTICS:

    S.NoVCE = V VCE = V VCE = V

    VBE (V) IB (A) VBE (V) IB (A) VBE (V) IB (A)

    OUTPUT CHARACTERISTICS:

    S.NoIB = A IB = A IB = A

    VCE (V) IC (mA) VCE (V) IC (mA) VCE (V) IC (mA)

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    3. Reverse Voltage Gain (hre) =

    , IB = constant

    4. Output Conductance (hoe) =

    , IB = constant

    Result:

    Thus the input and output characteristics of the given BJT were obtained for CE

    configuration.

    Input Impedance (hie) =

    Forward Current Gain (hfe) =

    Reverse Current Gain (hre) =

    Output Conductance (hoe) =

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    CHARACTERISTICS OF CB CONFIGURATION

    CIRCUIT DIAGRAM:

    INPUT CHARACTERISTICS:

    OUTPUT CHARACTERISTICS:

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    Expt.No:8

    CHARACTERISTICS OF CB CONFIGURATION

    Aim:

    To plot the input and output characteristics of a given BJT in CB configuration and

    determine its hybrid parameters.

    Components Required:

    S.No Components/Equipments Range Quantity

    1 Bipolar Junction Transistor BC 107 1

    2 Ammeter (0-30)mA 2

    3 Voltmeter (0-5)V

    (0-25)V

    1

    1

    4 Resistor 100 1

    5 RPS (0-15)V 2

    6 Connecting Wires As Reqd.,

    Theory:

    In CE configuration, the emitter is taken as input terminal, collector is taken as output

    terminal and base is taken as common terminal. The input characteristics are drawn for different

    values of IE and VBE with VCB constant. The output characteristics are drawn for different values

    of IC and VCB with IE constant.

    Procedure:

    1. Make connections as per the circuit diagram.2. To obtain the input characteristics, keep the value of VCB constant. For different

    values of VBE, tabulate the corresponding values of IE.

    3. Repeat the procedure for various constant values of VCB.4. Plot the graph and calculate the hybrid parameters.5. To obtain the output characteristics, keep the value of IE constant. For different values

    of VCB, tabulate the corresponding values of IC.

    6. Repeat the procedure for various constant values of IE.7. Plot the graph and calculate the hybrid parameters.

    Formula Used:

    1. Input Impedance (hib) =

    , VCB = constant

    2. Forward Current Gain (hfb) =

    , VCB = constant

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    PIN DIAGRAM SYMBOL

    TABULATION:

    INPUT CHARACTERISTICS:

    S.NoVCB = V VCB = V VCB = V

    VEB (V) IE (mA) VEB (V) IE (mA) VEB (V) IE (mA)

    OUTPUT CHARACTERISTICS:

    S.NoIE = mA IE = mA IE = mA

    VCB (V) IC (mA) VCB (V) IC (mA) VCB (V) IC (mA)

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    CHARACTERISTICS OF UJT

    CIRCUIT DIAGRAM:

    CHARACTERISTIC CURVE: Symbol Pin Diagram

    TABULATION:

    S.No

    VB1B2 = (V) VB1B2 = (V)

    VB1E (V) IE (mA) VB1E (V) IE (mA)

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    Expt.No.9

    CHARACTERISTICS OF UJT AND SCR

    Aim:

    To obtain the characteristics of UJT and SCR.

    Components Required:

    S.No Components/Equipments Range Quantity

    1 UJT 2N2646 1

    2 SCR 2P4M 1

    3 Resistor 1K

    470

    330

    11

    1

    4 RPS (0-5)V 2

    5 Ammeter (0-20)mA

    (0-100)mA

    1

    1

    6 Voltmeter (0-5)V(0-20)V

    11

    7 Connecting Wires As Reqd.,

    UJT

    Theory:

    UJT is a three terminal semiconductor switching device. As it has one PN junction, it is

    called Uni Junction Transistor. The heavily doped P region is called emitter E and lightly doped

    n region constitute base B1 and B2. The negative resistance property of UJT enables it to be

    employed in various applications namely relaxation oscillator, sawtooth generator, switching,

    timing and phase control circuits.

    Procedure:

    1. Connect the circuit as per the circuit diagram.2. Vary the value of input voltage and note down the corresponding emitter current IE and

    VBE with VB1B2 constant.

    3. Plot the graph with VBE against IE.4. Calculate the intrinsic stand-off ratio using formula.

    Formula Used:

    1. Intrinsic Stand-off ratio, = Intrinsic stand-off ratio = (VP-VD)/VB1B22. Negative Resistance =

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    CHARACTERISTICS OF SCR

    CIRCUIT DIAGRAM:

    CHARACTERISTICS CURVE: SYMBOL

    PIN DIAGRAM

    TABULATION:

    Before Triggering:

    IG = mA

    VAK(V) IA (mA)

    After Triggering:

    IG = mA

    VAK(V) IA (mA)

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    SCR

    Theory:

    SCR is a four layer PNPN device. It is a rectifier with a control element. It has three

    diodes connected back to back. It is widely used as a switching device in power control

    applications. It has three terminals namely Anode (A), Cathode (K) and Gate (G). The gate

    controls the firing of the SCR.

    Procedure:

    1. Connections are made as per the circuit diagram.2. Keep IG = 0mA.3. Vary the power supply and note down the anode to cathode voltage V AK and the anode

    current IA.

    4. Increase the gate current till the SCR gets triggered and keep IG constant.5. Now vary the power supply and note down the corresponding anode to cathode voltage

    VAKand the anode current IA.6. Note down the holding current IH and break-over voltage (VBO).7. Plot the graph.

    Result:

    Thus the characteristics of UJT and SCR were obtained.

    SCR:

    Holding Current IH =

    Break-over Voltage VBO =

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    CHARACTERISTICS OF JFET

    CIRCUIT DIAGRAM:

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    Expt.No.10

    CHARACTERISTICS OF JFET AND MOSFET

    Aim:

    To determine and plot the drain and transfer characteristics of the given JFET and

    MOSFET

    Components Required:

    S.No Components/Equipments Range Quantity

    1 JFET BFW10 1

    2 MOSFET 1

    3 Resistor 1K 1

    4 RPS (0-10)V 1

    5 Ammeter (0-15)mA

    (0-50)mA

    1

    1

    6 Voltmeter (0-3)V

    (0-10)V(0-25)V

    (0-30)V

    1

    11

    1

    7 Connecting Wires As Reqd.,

    JFET

    Theory:

    FET is a semiconductor switching device in which the flow of electron in the

    conducting region is controlled by an external electric field. As current conduction is only

    by majority carriers, FET is said to be a unipolar device.

    A Junction Field Effect Transistor (JFET) has three terminals namely source (S),

    Drain (D) and Gate (G). Source S is connected to negative of the battery. Drain D isconnected to positive of the battery. A PN junction is formed which is the Gate G.

    Procedure:

    1. Connect the circuit as per the circuit diagram.2. To obtain drain characteristics:

    i. Keep voltage VGS constant.ii. Increase the voltage VDS in a number of steps and note the corresponding

    drain current ID.

    iii. Repeat the procedure for various constant values of VGS.iv. Plot the graph with VDS against ID.

    3. To obtain transfer characteristics:i. Keep the voltage VDS constant.

    ii. Increase the voltage VGS in a number of steps and note the correspondingdrain current ID.

    iii. Repeat the procedure for various constant values of VDS.iv. Plot the graph with VGS against ID for various constant values of VDS.

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    TABULATION:

    Drain Characteristics:

    S.NoVGS = (V) VGS = (V)

    VDS (V) ID (mA) VDS (V) ID (mA)

    Transfer Characteristics:

    S.NoVDS = (V) VDS = (V)

    VGS (V) ID (mA) VGS (V) ID (mA)

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    v. Determine the values of drain resistance, transconductance, amplificationfactor, pinch-off voltage and drain-source saturation current.

    Formula Used:

    1. Drain Resistance, rd = VDS / ID , VGS = constant2. Trans-conductance, gm = ID / VGS , VDS = constant3. Amplification factor, = rd * gm

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    CHARACTERISTICS OF MOSFET

    CIRCUIT DIAGRAM:

    DRAIN CHARACTERISTICS TRANSFER CHARACTERISTICS

    SYMBOL PIN DIAGRAM

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    MOSFET

    Theory:

    Metal-Oxide-Semiconductor Field Effect Transistor (MOSFET) is also called Insulated

    Gate Field Effect Transistor (IGFET). MOSFET can be of two types namely depletion type

    MOSFET and enhancement type MOSFET. MOSFET has only one P region which is called

    substrate (SS). The Gate (G) is insulated from the conducting channel by metal oxide insulating

    film. When a negative bias is applied at the gate, it acts as depletion MOSFET and when a

    positive bias is applied at the gate, it acts as enhancement type MOSFET.

    Procedure:

    1. Connect the circuit as per the circuit diagram.2. To obtain drain characteristics:

    i. Keep voltage VGS constant.ii. Increase the voltage VDS in a number of steps and note the corresponding

    drain current ID.iii. Repeat the procedure for various constant values of VGS.iv. Plot the graph with VDS against ID.

    3. To obtain transfer characteristics:i. Keep the voltage VDS constant.

    ii. Increase the voltage VGS in a number of steps and note the correspondingdrain current ID.

    iii. Repeat the procedure for various constant values of VDS.iv. Plot the graph with VGS against ID for various constant values of VDS.

    4. Determine the values of drain resistance, transconductance, amplification factor,pinch-off voltage and drain-source saturation current.

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    TABULATION:

    Drain Characteristics:

    S.NoVGS = (V) VGS = (V)

    VDS (V) ID (mA) VDS (V) ID (mA)

    Transfer Characteristics:

    S.NoVDS = (V) VDS = (V)

    VGS (V) ID (mA) VGS (V) ID (mA)

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    Result:

    Thus the characteristics of JFET and MOSFET were obtained.

    JFET:

    Drain resistance, rd =

    Transconductance, gm =

    Amplification factor, =

    Pinch-off voltage, VP =

    Drain-source Saturation Current IDSS =

    MOSFET:

    Drain resistance, rd =

    Transconductance, gm =

    Amplification factor, =

    Drain-source Saturation Current IDSS =

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    CHARACTERISTICS OF DIAC

    CIRCUIT DIAGRAM:

    MT1 negative with respect to MT2 V-I CHARACTERISTICS

    MT2 negative with respect to MT1 VBO

    TABULATION:

    MT1 positive with respect to MT2

    S.NoVoltage V

    (V)

    Current I

    (mA)

    MT2 positive with respect to MT1

    S.NoVoltage V

    (V)

    Current I

    (mA)

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    Expt.No:11

    CHARACTERISTICS OF DIAC AND TRIAC

    Aim:

    To determine the characteristics of the given DIAC and TRIAC.

    Components Required:

    S.No Components/Equipments Range Quantity

    1 DIAC DB3 1

    TRIAC BT136 1

    2 Resistor 1K 1

    3 RPS (0-60)V 1

    4 Ammeter (0-10)mA

    (0-50)mA

    (0-100)mA MC

    1

    1

    1

    5 Voltmeter (0-15)V

    (0-100)V MC

    1

    1

    6 Connecting Wires As Reqd.,

    DIAC

    Theory:

    A diac is a two terminal bidirectional semiconductor device that can be switched from

    OFF state to ON state for either polarity of applied voltage. When a positive or negative voltage

    is applied across the terminals, a small amount of leakage current flows. As the applied voltage

    is increased, the leakage current will continue to flow until the voltage reaches the break-over

    voltage VBO. At this point, avalanche breakdown occurs and the device exhibits negative

    resistance.

    Procedure:

    1. Connect the circuit as per the circuit diagram.2. MT1 is kept positive with respect to MT2.3. Vary the supply voltage and note down the corresponding voltmeter and ammeter

    readings.

    4. Plot the graph with V against I.5. Repeat the procedure with MT2 kept negative with respect to MT1.

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    CHARACTERISTICS OF TRIAC

    CIRCUIT DIAGRAM:

    V-I CHARACTERISTICS:

    TABULATION:

    S.No

    IG1= (mA) IG2 = (mA)

    VAK(V) IA (mA) VAK(V) IA (mA)

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    TRIAC

    Theory:

    A TRIAC is a three terminal semiconductor switching device which can control

    alternating current in a load. It consist of 2 SCRs connected in anti-parallel, so its characteristics

    in I and III quadrants are essentially identical to those of an SCR in the I quadrant. The TRIAC

    can be operated with either positive or negative gate control voltage, but in normal operation

    usually the gate voltage is positive in I quadrant and negative in III quadrant. The supply voltage

    at which the TRIAC is turned ON depends on the gate current. The greater the gate current, the

    smaller the supply voltage at which the TRIAC is turned ON.

    Procedure:

    1. Connect the circuit as per the circuit diagram.2. To set the gate current IG, set VMT1, VMT2 and vary VG till VAK suddenly drops. Note

    down the corresponding gate current IG.

    3.

    Set the gate current equal to firing current and vary the anode to cathode voltage.4. Vary VAKin steps and note down the corresponding ammeter readings.5. Open the gate terminal and decrease VAK.6. Plot the graph.

    Result:

    Thus the characteristics of DIAC and TRIAC were determined.

    DIAC:


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