Capacitors are a key
component in a circuit designer’s tool kit, thus a short discussion
on evaluating their affect on circuit performance is in order.
Capacitors have an impedance of XC = 1/2πfC. Note that when the
frequency is zero the capacitive impedance (also known as reactance)
is infinite, and that when the frequency is infinite the capacitive
impedance is zero. These end-points are derived from the final value
theorem, and they are used to get a rough idea of the effect of a
capacitor. When a capacitor is used with a resistor, they form what
is called a break-point. Without going into complicated math, just
accept that the break frequency occurs at f = 1/(2π RC) and the gain
is –3 dB at the break frequency.
The low pass filter
circuit shown in Figure 3–10 has a capacitor in parallel with the
feedback resistor. The gain for the low pass filter is given in
Equation 3–20.
Figure 3–10.
Low-Pass Filter
At very low
frequencies XC ⇒ ∞, so RF dominates
the parallel combination in Equation 20, and the capacitor has
no effect. The gain at low frequencies is –RF/RG. At very high
frequencies XC ⇒ 0, so the feedback
resistor is shorted out, thus reducing the circuit gain to
zero. At the frequency where XC = RF the gain is reduced by √2
because complex impedances in parallel equal half the vector sum of
both impedances.
Connecting the
capacitor in parallel with RG where it has the opposite effect makes
a high pass filter (Figure 3–11). Equation 3–21 gives the
equation for the high pass filter.
Figure
3–11.High-Pass Filter
At very low
frequencies XC ⇒ ∞, so RG dominates
the parallel combination in Equation 3–21, and the capacitor
has no effect. The gain at low frequencies is 1+RF/RG. At very high
frequencies XC ⇒ 0, so the gain setting
resistor is shorted out thus increasing the circuit gain to
maximum.
This simple
technique is used to predict the form of a circuit transfer function
rapidly. Better analysis techniques are presented in later chapters
for those applications requiring more precision.
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