Characteristics of JFETS

CHARACTERISTICS OF JFETS

There are two types of static characteristics viz

(1) Output or drain characteristic and

(2) Transfer characteristic.

1. Output or Drain Characteristic. The curve drawn between drain current I_p and drain-source voltage V_DS with gate-to source voltage V_GS as the parameter is called the drain or output characteristic. This characteristic is analogous to collector characteristic of a BJT:

JFET Drain Characteristic With Shorted-Gate

(a) Drain Characteristic With Shorted-Gate. The circuit diagram for determining the drain characteristic with shorted-gate for an N-channel JFET is given in figure. and the drain characteristic with shorted-gate is shown in another figure.

Initially when drain-source voltage V_ns is zero, there is no attracting potential at the drain, so no current flows inspite of the fact that the channel is fully open. This gives drain current Ip = 0. For small applied voltage V_na, the N-type bar acts as a simple semiconductor resistor, and the drain current increases linearly with_the increase in Vds, upto the knee point. This region, (to the left of the knee point) of the curve is called the channel ohmic region, because in this region the FET behaves like an ordinary resistor.

With the increase in drain current I_D, the ohmic voltage drop between the source and channel region reverse-biases the gate junction. The reverse-biasing of the gate junction is not uniform throughout., The reverse bias is more at the drain end than that at the source end of the channel, so with the increase in Vds, the conducting portion of the channel begins to constrict more at the drain end. Eventually a voltage Vds is reached at which the channel is pinched off. The drain current I_D no longer increases with the increase in Vds. It approaches a constant saturation value. The value of voltage V_DS at which the channel is pinched off (i.e. all the free charges from the channel get removed), is called the pinch-off voltage V_p. The pinch-off voltage Vp, not too sharply defined on the curve, where the drain current I_D begins to level off and attains a constant value. From point A (knee point) to the point B (pinch-off point) the drain current I_D increases with the increase In voltage V_ds following a reverse square law. The region of the characteristic in which drain current I_D remains fairly constant is called the pinch-off region. It is also sometimes called the saturation region or amplifier region. In this region the JFET operates as a constant current device since drain current (or output current) remains almost constant. It is the normal operating region of the JFET when used as an amplifier. The drain current in the pinch-off region with V_GS = 0 is referred to the drain-source saturation current, Idss).

It is to be noted that in the pinch-off (or saturation) region the channel resistance increases in proportion to increase in V_DS and so keeps the drain current almost constant and the reverse bias required by the gate-channel junction is supplied entirely by the voltage drop across the channel resistance due to flow of I_Dsg and not by the external bias because V_GS = 0

Drain current in the pinch-of region is given by Shockley’s equation

where I_D is the drain current at a given gate-source voltage V_GS, I_DSS is the drain-current with gate shorted to source and V_GS (_0FF) is the gate-source cut-off voltage.

If drain-source voltage, Vds is continuously increased, a stage comes when the gate-channel junction breaksdown. At this point current increases very rapidly. and the JFET may be destroyed. This happens because the charge carriers making up the saturation current at the gate channel junction accelerate to a high velocity and produce an avalanche effect.

JFET-Drain Characteristics With External Bias

Drain Characteristics With External Bias: The circuit diagram for determining the drain characteristics with different values of external bias is shown in figure. and a family of drain characteristics for different values of gate-source voltage V_GS is given in next figure

It is observed that as the negative gate bias voltage is increased

(1) The maximum saturation drain current becomes smaller because the conducting channel now becomes narrower.

(2) Pinch-off voltage is reached at a lower value of drain current I_D than when V_GS = 0. When an external bias of, say – 1 V is applied between the gate and the source, the gate-channel junctions are reverse-biased even when drain current, I_D is zero. Hence the depletion regions are already penetrating the channel to a certain extent when drain-| source voltage, V_DS is zero. Due to this reason, a smaller voltage drop along the channel (i.e. smaller than that for V_GS = 0) will increase the depletion regions to the point where 1 they pinch-off the current. Consequently, the pinch-off voltage V_P is reached at a lower 1 drain current, I_D when V_GS = 0.

(3) The ohmic region portion decreases.

(4) Value of drain-source voltage V_DS for the avalanche breakdown of the gate junction is reduced.

Value of drain-source voltage, V_DS for breakdown with the increase in negative bias voltage is reduced simply due to the fact that gate-source voltage, V_GS keeps adding to the I reverse bias at the junction produced by current flow. Thus the maximum value of V_{DS I that can be applied to a FET is the lowest voltage which causes avalanche breakdown. It is also observed that with VGS = 0, ID saturates at IDSS and the characteristic shows VP = 4 V. When an external bias of – 1 V is applied, the gate-channel junctions still require -4 V to achieve pinch-off. It means that a 3 V drop is now required along the channel instead of the previous 4.0 V. Obviously, this drop of 3 V can be achieved with a lowervalue of drain current, Similarly when VGS = – 2 V and – 3 V, pinch-off is achieved with 2 V and 1 V respectively, along the channel. These drops of 2 V and 1 V are, of course, achieved with further reduced values of drain current, ID. It is further observed that when the gate-source bias is numerically equal to pinch-off voltage, VP (-4 V in this case), no channel drop is required and, therefore, drain current, ID is zero. The gate-source bias voltage required to reduce drain current, ID to zero is designated the gate-source cut-off voltage, VGS /0FF) and, as explained,}

Hence for working of JFET in the pinch-off or active region it is necessary that the following conditions be fulfilled.

V_P < V_DS < V_{DS (max)}

V_{GS (OFF)} < V_GS < 0

0 < I_D < I_DSS

jfet-transfer-characteristic

2. Transfer Characteristic of JFET

The transfer characteristic for a JFET can be determined experimentally, keeping drain-source voltage, V_DS constant and determining drain current, I_D for various values of gate-source voltage, V_GS. The circuit diagram is shown in fig. 9.7 (a). The curve is plotted between gate-source voltage, V_GS and drain current, I_D, as illustrated in fig. 9.8. It is similar to the transconductance characteristic of a vacuum tube or a transistor. It is observed that

(i) Drain current decreases with the increase in negative gate-source bias

(ii) Drain current, I_D = I_DSS when V_GS = 0

(iii) Drain current, I_D = 0 when V_GS = V_D The transfer characteristic follows equation (9.1)

The transfer characteristic can also be derived from the drain characteristic by noting values of drain current, I_D corresponding to various values of gate-source voltage, V_GS for a constant drain-source voltage and plotting them.

It may be noted that a P-channel JFET operates in the same way and have the similar characteristics as an N-channel JFET except that channel carriers are holes instead of electrons and the polarities of V_GS and V_DS are reversed.

jfet-geometry

MERITS AND DEMERITS OF JFETS

Junction field effect transistors combine several merits of both conventional (or bipolar) transistors and vacuum tubes. Some of these are enumerated below:

1. Its operation depends upon the flow of majority carriers only, it is, therefore, a unipolar (one type of carrier) device. On the other hand in an ordinary transistor both majority and minority carriers take part in conduction and, therefore, ordinary transistor is sometimes called the bipolar transistor. The vacuum tube is another example of a unipolar device. ‘

2. It is simpler to fabricate, smaller in size, rugged in construction and has longer life and higher efficiency. Simpler to fabricate in IC form and space requirement is also lesser.

3. It has high input impedance (of the order of 100 M Q), because its input circuit (gate to source) is reverse biased, and so permits high degree of isolation between the input and the output circuits. However, the input circuit of an ordinary transistor is forward biased and, therefore, ordinary transistor has low input impedance.

4.It carries very small current because of reverse biased gate and, therefore, it operates just like a vacuum tube where control grid (corresponding to gate in JFET) carries extremely small current and input voltage controls the output current. This is the reason that JFET is essentially a voltage driven device (ordinary transistor is a current operated device since input current controls the output current.)

5.    An ordinary transistor uses a current into its base for controlling a large current between collector and emitter whereas in a JFET voltage on the gate (base) terminal is used for controlling the drain current (current between drain and source). Thus an ordinary transistor gain is characterized by current gain whereas the JFET gain is characterized as the transconductance (the ratio of drain current and gate-source voltage).
6.    JFET has no junction like an ordinary transistor and the conduction is through bulk material current carriers (N-type or P-type semiconductor material) that do not cross junctions. Hence the inherent noise of tubes (owing to high temperature operation) and that of ordinary transistors (owing to junction transitions) is not present in JFET.
7.    It is relatively immune to radiation.    .
8.    It has negative temperature coefficient of resistance and, therefore, has better thermal stability.
9.    It has high power gain and, therefore, the necessity of employing driver stages is eliminated.

10.    It exhibits no offset voltage at zero drain current and, therefore, makes an excellent signal chopper.
11.    It has square law characteristics and, therefore, it is very useful in the tuners of radio and TV receivers.
12.    It has got high frequency response.

The main drawback of JFET is
1. Its relative small gain-bandwidth product in comparison with that of a conventional transistor.
2. Greater susceptibility to damage in its handling.
3. JFET has low voltage gains because of small transconductance .
4. Costlier when compared to BJT’s

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