Use Kirchhoff's Laws and the characteristic equation for a transformer in the circuit below to prove Eq. 6.78.
Use Kirchhoff's Laws and the characteristic equation for a transformer in the circuit below to prove Eq. 6.78.
Introductory Circuit Analysis (13th Edition)
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ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
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
Transcribed Image Text:1:0
ZMS
83
V
ZEB
F
Figure 6.14. Equivalent circuit for a linear reciprocal transducer using impedance parameters.
ZMs = ZMo(1 - k2)
(6.78)
where ZMs is defined as the short-circuit mechanical impedance, given by
FIU when V is zero, and the electromechanical coupling constant ke is given
by
TEM
ZEBZMO
(6.79)
Thus far, it seems we have manipulated a set of equations and then forced
a circuit model to match themn. That is exactly what we have done! When
we examine the linearization of nonlinear systems in the next chapter, we shall
apply this formulation to the electrostatic transducer of this chapter, which will
provide some intuition about the meaning of these symbols. In the mean time,
this exercise provides good opportunity for practice in manipulating circuits
that contain two-nort elements.
6.5 Use Kirchhoff's Laws and the characteristic equation for a transformer
in the circuit below to prove Eq. 6.78.
1:0
ZMS
ZEB
88 F2
V
F
ZMs =
Zмо(1 - к)
(6.78)
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