Widlar current source

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Widlar current source.
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Widlar current source.

A Widlar current source is a current source attributed to the late Bob Widlar, in which an emitter degeneration resistor is only applied to Q2 (designated as R2 in the schematic). This has the effect of turning off Q2 relative to Q1. The current source is commonly used to generate low currents. Analysis is as follows,

Assume that both transistors have the same current gain β.

Neglecting the base current of Q2, the output current IC2 is also the current through R2. Hence,

VBE1 = VBE2 + IC2R2 ... (1)

Since in general the base-emitter voltage is given by,

V_{BE} = V_T\ ln\left(\frac{I_C}{I_S}\right) ... (2)

Rearranging (1),

IC2R2 = VBE1VBE2 ... (3)

Substituting for VBE from (2) into (3) we get,

I_{C2}R2 = V_T\ ln\left(\frac{I_{C1}}{I_{S}}\right) - V_T\ ln\left(\frac{I_{C2}}{I_{S}}\right) ... (4)

= V_T\left[ln\left(\frac{I_{C1}}{I_S}\right) - ln\left(\frac{I_{C2}}{I_S}\right)\right] ... (5)

So,

I_{C2} = \frac{V_T}{R2}ln\left(\frac{I_{C1}}{I_{C2}}\right) ... (6)

The current through R1 is the input or reference current given as,

IR1 = IC1 + IB1 + IB2 ... (7)

= I_{C1} + \frac{I_{C1}}{\beta} + \frac{I_{C2}}{\beta} ... (8)

If β is large, the last two terms of the above equation can be neglected. Hence,

I_{R1} \approx I_{C1}

Thus assuming the forwared base-emitter voltage of Q1 to be 0.7 V,

I_{C1} \approx I_{R1} = \frac{V_{CC} - 0.7}{R1} ... (9)

Substituting (9) in (6) we get,

I_{C2} = \frac{V_T}{R2}ln\left(\frac{I_{R1}}{I_{C2}}\right) =  \frac{V_T}{R2}ln\left(\frac{V_{CC} - 0.7}{I_{C2}R1}\right) ... (10)

The above equation is the approximate solution for the output current IC2 and is non-linear. An iterative process has to be employed to arrive at a value for R1 which gives a value of IC2 which is reasonably close to that desired.

Knowing the desired values of IC1 and IC2, R2 can be easily calculated.

Note that with the circuit as shown, if VCC changes, the output current will change. Hence the circuit must be driven by a constant current source instead of R1 to keep the output current constant.

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