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2.3 Circuits and Subcircuits 57<br />

In[7]:= eqAmpSimple = CircuitEquations[flatAmpSimple];<br />

DisplayForm[eqAmpSimple]<br />

Out[8]//DisplayForm=<br />

1<br />

<br />

R1 <br />

1<br />

R2<br />

<br />

1<br />

R1<br />

0 0 0 1 0 1 <br />

1 1<br />

<br />

R1<br />

<br />

R1 <br />

1<br />

RC<br />

<br />

1<br />

RC<br />

0 0 0 1 0<br />

0 1 1<br />

<br />

RC<br />

<br />

RC<br />

0 0 0 0 beta<br />

1<br />

0 0 0 <br />

RB <br />

1<br />

RE<br />

<br />

1<br />

RB<br />

0 0 beta .<br />

0 0 0 <br />

1 1<br />

RB<br />

<br />

RB<br />

0 0 1<br />

1 0 0 0 0 0 0 0<br />

<br />

0 1 0 0 0 0 0 0<br />

<br />

1 0 0 0 1 0 0 0 <br />

V$1 0 <br />

V$2<br />

0<br />

V$3<br />

0<br />

V$4<br />

0<br />

⩵⩵<br />

V$X$Q1 0<br />

I$V1 1<br />

I$VCC 0<br />

<br />

<br />

IC$CC$Q1 0 <br />

To compute the small-signal voltage transfer function we must solve the MNA equations for the<br />

node voltage V$3 at the output node 3.<br />

In[9]:= v3 = Solve[eqAmpSimple, V$3]<br />

beta RC<br />

Out[9]= V$3 <br />

RB RE beta RE <br />

The following command extracts the symbolic transfer function expression from the return value of<br />

Solve.<br />

In[10]:= vtf = V$3 /. First[v3]<br />

beta RC<br />

Out[10]= <br />

RB RE beta RE<br />

Now, let’s see what happens when we make the (usually realistic) assumption that the transistor<br />

current gain is very large:<br />

In[11]:= Limit[vtf, beta −> Infinity]<br />

Out[11]= RC <br />

RE<br />

The above result is indeed identical to the well-known approximate formula for the voltage gain of<br />

a common-emitter amplifier. Doing the same calculations for the other transistor model shall be left<br />

to the reader as an exercise.

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