Consoles 881
25.11.11 The Bootstrap
The simplest fake inductor is shown in Fig. 25-63A,
with typical values. It relies on a technique called boot-
strapping. The principles are shown in Fig. 25-62. A
1k: resistor with 1 V across it will pass 1 mA. Without
changing the source potential of 1 V, the bottom end of
the resistor is tied to 0.8 V. There is 0.2 V across the
resistor, and so a current of 0.2 mA flows through the
resistor. The source (still at 1 V) sees 0.2 mA flowing
away from it, the amount of current it would expect to
see going to a 5 k: resistor value (1 V/0.2 mA = 5 k:).
It thinks it’s looking at a 5 k: resistor! Continuing this,
stuffing a potential of 1 V (not the same source) at the
bottom end of the resistor means there is no voltage
across the resistor, so there is no current flow. Our orig-
inal source thinks it’s seeing an open circuit (infinite
resistance) despite the fact that there is still a definite,
real, physical 1 k: resistor hanging on it.
This phenomenon holds true with any source
voltage, ac or dc, provided the instantaneous bootstrap
voltage is the same as the source. Any phase or potential
difference creates an instantaneous potential difference
across the resistor; current flows and an apparent resis-
tance materializes.
This fake inductor works on frequency-dependent
Figure 25-61. Totem-pole gyrators. bootstrapping, the terminal being almost totally boot-
E. Input/output response of D.
A. Totem pole gyrator with typical values.
B. High-pass filter.
C. Input output response of B.
D. Bandpass filter.
Q approximately 30
Loss indicates
dynamic impedance
@ 20 k 7
Totem pole
Totem pole
as shown
10 k 7
10 k 7
10 k 7
10 k 7
1 k 7
(C1)
0.1 MF
0.1 MF
100 Hz 1 kHz 10 kHz
Frequency
100 Hz 1 kHz 10 kHz
0
10 dB
20 dB
0.1 MF
10 k 7
V 0
V 0
+ 40dB
+20 dB
0
10 dB
Figure 25-62. Bootstrapping analysis.
Main
terminal
Terminal sees
Zero volts
ground
No current Opencircuit
Note: 1 k 7 resistor is attached
to terminal in all cases
1 k (^7) 1 mA
1V
1 k (^7) 0.2 mA
1V
0.8 mA
1V
1 k 7
1V
5 k 7
1 k 7