In an L-R-C series circuit, R = 150 Ω, L = 0.750 H, and C = 0.0180 μ F. The source has voltage amplitude V = 150 V and a frequency equal to the resonance frequency of the circuit, (a) What is the power factor? (b) What is the average power delivered by the source? (c) The capacitor is replaced by one with C = 0.0360 μ F and the source frequency is adjusted to the new resonance value. Then what is the average power delivered by the source?
In an L-R-C series circuit, R = 150 Ω, L = 0.750 H, and C = 0.0180 μ F. The source has voltage amplitude V = 150 V and a frequency equal to the resonance frequency of the circuit, (a) What is the power factor? (b) What is the average power delivered by the source? (c) The capacitor is replaced by one with C = 0.0360 μ F and the source frequency is adjusted to the new resonance value. Then what is the average power delivered by the source?
In an L-R-C series circuit, R = 150 Ω, L = 0.750 H, and C = 0.0180 μF. The source has voltage amplitude V = 150 V and a frequency equal to the resonance frequency of the circuit, (a) What is the power factor? (b) What is the average power delivered by the source? (c) The capacitor is replaced by one with C = 0.0360 μF and the source frequency is adjusted to the new resonance value. Then what is the average power delivered by the source?
Part A
m
2πkT
) 3/2
Calculate the integral (v) = f vƒ (v)dv. The function f(v) describing the actual distribution of molecular speeds is called the Maxwell-Boltzmann distribution,
=
ƒ(v) = 4π (· v²e-mv²/2kT
. (Hint: Make the change of variable v² =x and use the tabulated integral foxne
integer and a is a positive constant.)
Express your answer in terms of the variables T, m, and appropriate constants.
-ax dx
n!
-
an+1
where n is a positive
(v)
=
ΕΠΙ ΑΣΦ
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