University Physics (14th Edition)
University Physics (14th Edition)
14th Edition
ISBN: 9780133969290
Author: Hugh D. Young, Roger A. Freedman
Publisher: PEARSON
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Chapter 31, Problem 31.66P

DATA You are given this table of data recorded for a circuit that has a resistor, an inductor with negligible resistance, and a capacitor, all in series with an ac voltage source:

f(Hz) 80 160
z (Ω) 15 13
ϕ (°) –71 67

Here f is the frequency of the voltage source, Z is the impedance of the circuit, and ϕ is the phase angle. (a) Use the data at both frequencies to calculate the resistance of the resistor. (Hint: Use the results of Exercise 31.21.) Calculate the average of these two values of the resistance, and use the result as the value of R in the rest of the analysis. (b) Use the data at 80 Hz and 160 Hz to calculate the inductance L and capacitance C of the circuit. (c) What is the resonance frequency for the circuit, and what are the impedance and phase angle at the resonance frequency?

31.66 IDENTITY and SET UP: For an L-R-C series circuit, tan ϕ = ω L 1 ω C R and the power factor is cosϕ = R/Z.

EXECUTE: (a) cosϕ = R/Z, so R = Z cosϕ.

At 80 Hz: R = (15 Ω) cos(−71°) = 4.88 Ω

At 160 Hz: R = (13 Ω) cos(67°) = 5.08 Ω

The average resistance is (4.88 Ω + 5.08 Ω)/2 = 5.0 Ω

(b) We use tan ϕ = ω L 1 ω C R with R = 5.0 Ω from part (a).

At 80 Hz: tan ( 71 ) = 2 π ( 80  Hz ) L 1 2 π ( 80  Hz ) C 5.0   Ω .

−14.52 = 160π Hz L − 1/[(160π Hz)C]. Eq. (1)

At 160 Hz: tan ( 67 ) = 2 π ( 160  Hz ) L 1 2 π ( 160  Hz ) C 5.0   Ω .

11.78 = 320π Hz L − 1/[(320π Hz)C]. Eq. (2)

Multiply Eq. (1) by −2 and add it to Eq. (2), giving 2(14.52) + 11.78 = (1/C)(1/80π − 1/320π).

C = 7.31 × 10−5 F, which rounds to C = 73 μF.

Substituting this result into either Eq. (1) or Eq. (2) gives L = 25.3 mH, which rounds to L = 25 mH.

(c) The resonance angular frequency is ω 0 = 1 L C , so the resonance frequency is

f 0 = ω 0 2 π = 1 2 π L C = 1 2 π ( 2.53 × 10 2  H ) ( 73.1 × 10 6  F ) = 117  Hz

At resonance, Z = R = 5.0 Ω and ϕ = 0.

EVALUATE: It is only at resonance that Z = R, not at the other frequencies.

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Chapter 31 Solutions

University Physics (14th Edition)

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