EXPERIMENT NO. 7: FIELD EFFECT TRANSISTOR

OBJECTIVE

To measure the characteristics of a junction field effect transistor (JFET) and to test a simple votage amplifier.

APPARATUS

Circuit Module No. "Exp. 7"

This circuit uses a p-channel junction field effect transistor 2N4360 for which the drain characteristics are shown below.

Note that the characteristics vary substantially with temperature and from device to device.

The circuit of Figure 1 illustrates a simple FET amplifier with dc supplies connected in the drain and the gate circuits.


Figure 1

The function of the 470 Ohm resistor is to allow the gate bias voltage VGG to be applied to the gate of the FET without short circuiting the signal source. Other methods of biasing are possible and these can result in the elimination of the supply voltage VGG.

Neglecting RL, and the 100µF capacitor, we can write the equation

VDD = RD + VDS or, rearranging iD = - VDS / RD + VDD / RD

This is the equation for the dc load line which can be drawn on the drain characteristics with a slope of -1/RD. The intercept on the iD axis is VDD / RD and on the VDS axis is VDD.

The dc load line give the pairs of values of ID and VDS that can exist in the circuit. The values that actually do exist are determined by the gate to source voltage VGS and known as the quiescent values ID and VDS. Varying VGS will cause VDS and ID to change.

If VGS is varied about its quiescent value, VGS will also vary about its quiescent value VDS. For sinusoidal voltages, the output voltage is 180° out of phase with the input voltage. When the input voltage swings to parts of the characteristics which deviate from a straight line the output will become more and more distorded.

One way of obtaining an insight into the voltage amplification process is to plot the output voltage VDS as a function of input voltage VGS for a fixed load resistance. Such a curve is known as a dynamic transfer characteristic. The small signal voltage gain can be estimated from the gradient of the plot of VDS against VGS.

Where a coupling capacitor is used at the output of an amplifier, the load on the circuit for the ac signal will be different to the load for the dc supply. The circuit in Figure 1 uses a 100µ coupling capacitor.

To analyse the circuit in this case, it is necessary to make use of the ac load line. The dc load is the reistor RD while the ac load is RL in parallel with RD so that the ac load line has a slope of -1/(RL || RD) and must pass through the quiescent or Q-point.

Note that it is necessary to plot new transfer characteristics to estimate the small signal transfer function when an ac load is applied.


Figure 2

PRELIMINARY:

  1. Taking VGG as 1.1V in Figure 1 and using the characteristics supplied, plot
  2. From the transfer characteristics: calculate and plot the small signal gain as a function of the bias voltage VGS for: Assume that a singla magnitude of ±½ a volt is sufficiently small to constitute a "small signal".
PROCEDURE:
  1. Connect the circuit as shown in Figure 3 with RD = 390 Ohm and RL =

    Set the supply voltage VDD to -15 volts and with VGS equal to 0 volts, vary VDS in steps down to zero volts tracing out the drain characteristics, ie. plot ID as a function of VDS for a fixed VGS. Plot the characteristics as you proceed.

  2. Repeat 1. above for VGS set in turn to 0.5, 1, 1.5, 2 volts.
  3. Connect the amplifier circuit shown in the Figure 1 with VGG = 1.1 volts, RD = 2.2 k but without the ac load resistor RL connected. Set the frequency of the oscillator to about 1000 Hz and initially have the amplitude control turned right down.

    View the output on a CRO. Advance the amplitude control on the oscillator until a sinusoidal output signal appears. Measure the voltage gain by displaying the input and output signals on the CRO.

  4. Repeat 3, with VGG of 0.5, 1 and 2 volts.
  5. Repeat 3 and 4 with an ac load of 2.2k connected.
  6. Increase the ac input voltage until severe distortion starts to occur. Sketch the output waveform.
REPORT:
  1. The report is to include:
  2. An essential feature of an amplifier is that some power gain is achieved.

Figure 3

DRAIN CHARACTERISTICS OF P-CHANNEL FIELD EFFECT TRANSISTOR 2N4360

For assistance in connecting up your circuit for this experiment, click on bar above.