B6, General Physics Experiment II ω LC Fall Semester, 2020 Name: Team No. : Department: Date : Student ID: Lecturer’s Signature : Introduction Goals Understand a forced oscillation and resonance. Measure the natural angular frequency (ω LC ) of a RLC circuit. Understand phase shifts among v R (t), v L (t), and v C (t). Make Lissajous curves with v R (t), v L (t), and v C (t). Theoretical Backgrounds 1. RLC circuit Consider a circuit consisting of a resistor of resistance R, a capacitor of capacitance C , an inductor of inductance L and an AC emf E : E (t)= E m sin ω d t. (a) The capacitive reactance is X C = 1 ω d C . (b) The inductive reactance is X L = ω d L. (c) The impedance is Z = R + j (X L - X C )= |Z |e jφ , where j ≡ √ -1 and |Z | is the absolute value for the impedance |Z | = p R 2 +(X L - X C ) 2 and the phase φ is given by φ = arctan Im[Z ] Re[Z ] = arctan X L - X C R . (d) The current of the RLC circuit is i(t)= I Z sin(ω d t - φ). (e) The amplitude I Z for the current is I Z = E m p R 2 +(X L - X C ) 2 . 2. Resonance frequency (a) The amplitude I Z (ω d ) for the current of the RLC circuit is maximized when |Z | is minimum. (b) This happens when the imaginary part of Z vanishes: Im[Z ]= X L - X C =0. (c) Substituting the ω dependence into X L and X C , we find that ω = 1 √ LC . (d) The resonance frequency f is f = 1 2π √ LC . 3. Phasor 2020 KPOPE All rights reserved. Korea University Page 1 of 5
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B6, General Physics Experiment II ωLC Fall Semester, 2020
Name:
Team No. :
Department:
Date :
Student ID:
Lecturer’s Signature :
Introduction
Goals
� Understand a forced oscillation and resonance.
� Measure the natural angular frequency (ωLC) ofa RLC circuit.
� Understand phase shifts among vR(t), vL(t), andvC(t).
� Make Lissajous curves with vR(t), vL(t), andvC(t).
Theoretical Backgrounds
1. RLC circuit
Consider a circuit consisting of a resistor ofresistance R, a capacitor of capacitance C, aninductor of inductance L and an AC emf E :
E (t) = Em sinωdt.
(a) The capacitive reactance is
XC =1
ωdC.
(b) The inductive reactance is
XL = ωdL.
(c) The impedance is
Z = R+ j(XL −XC) = |Z|ejφ,
where j ≡√−1 and |Z| is the absolute value
for the impedance
|Z| =√R2 + (XL −XC)2
and the phase φ is given by
φ = arctanIm[Z]
Re[Z]= arctan
XL −XC
R.
(d) The current of the RLC circuit is
i(t) = IZ sin(ωdt− φ).
(e) The amplitude IZ for the current is
IZ =Em√
R2 + (XL −XC)2.
2. Resonance frequency
(a) The amplitude IZ(ωd) for the current of theRLC circuit is maximized when |Z| isminimum.
(b) This happens when the imaginary part of Zvanishes:
Im[Z] = XL −XC = 0.
(c) Substituting the ω dependence into XL andXC , we find that