The improved one-BJT current-limiting supply is not much different than the primitive circuit, though its one additional resistor does change the circuit behavior. The improved circuit is shown below.
Analysis quickly proceeds by Thevenizing the base circuit and β-transforming the Thevenin base resistance to the emitter, resulting in the following equivalent circuit.
When the BJT is not saturated, the output current is a maximum of
where VBE(IO) = VBE(sc). Under light load, the BJT saturates and as with the previous circuit, VCB(oc)
where VEB(oc) corresponds to the minimum-current value. In the previous circuit this was VEB(oc) = 0.50 V at 1.3 μA.
Solve for Ri from the VO equation:
RB is found by substituting for Ri in the IO equation and solving;
To design, choose RB. Its choice is subject to the constraint that RE ≥ 0 Ω. The subtraction of the RE term in RB results in the maximum RB when RE = 0 Ω. Then for larger RE, RB must be less, and
Dependence of IO on β is minimized when δIO/δβ is minimum, or whenever RE >> (Ri ||RB )/( β + 1). This compares with what was found for the primitive one-BJT circuit. For this circuit, Ri makes the inequality easier to satisfy.
To test these equations, a design was carried out and built for IO = 20 mA using a 2N2907 BJT selected for a β of 150. The VEB were calculated using IS = 5 fA = 5x10–15 A. IS is difficult to obtain directly from the VBE (IC) curves in the parts data because those curves are not exactly exponential. They include the additional linear voltage contribution of series resistance - of re’, the ohmic emitter resistance, and rb’, the ohmic base resistance, referred to the emitter. Additional calculation from the curves leads to the conclusion that the total effective ohmic emitter resistance is about 0.5 Ω. If the VBE are calculated from the given IS then the values will be somewhat low, especially for the high-current value. The easiest and most accurate procedure for design is to read the two pairs of numbers off the VBE curves.
The values used in this design were
The resistor values calculate from the design formulas to be
The circuit was built with these standard +/-5 % parts values but this time a $1000 DMM (a Keithley 2000) was used to go through the 5 % resistor parts bins and select parts within about 0.1 % of these nominal values. Then
β dependence is reduced with RE six times that of the base-referred resistance, showing the role of Ri. Also,
The base divider was disconnected from the base and the measured voltage agreed with the above value in all digits. Then the $30 (DT-182) DMM was used to measure output current by placing it as an ammeter across the output, effectively shorting it. The DMMs were both used to measure voltages, and the following values resulted.
The measured value of V was 5.00 V. The measured values of IO appear to verify the design equations.
This improved one-BJT current-limited source is not a bad choice for a low-cost, low-parts-count current limiting supply extender. The value of IO, unlike the carefully value-selected prototype above, will have a spread of values corresponding to parts tolerances, including BJT β. Many less-demanding applications can be satisfied by it.
By adding one more transistor, some additional improvement can be realized, the topic we consider next.