62. A series RL circuit is connected to an emf source of angular frequency
. The current:
A) leads the applied emf by tan–1(
L/R)
B) lags the applied emf by tan–1(
L/R)
C) lags the applied emf by tan–1(
R/L)
D) leads the applied emf by tan–1(
R/L)
E) is zero
63. An RC series circuit is connected to an emf source having angular frequency
. The
current:
A) leads the source emf by tan–1(1/
CR)
B) lags the source emf by tan–1(1/
CR)
C) leads the source emf by tan–1(
CR)
D) lags the source emf by tan–1(
CR)
E) leads the source emf by /4
64. An RLC series circuit is driven by a sinusoidal emf with angular frequency
d. If
d is
increased without changing the amplitude of the emf, the current amplitude increases. If L is
the inductance, C is the capacitance, and R is the resistance, this means that:
A)
dL > 1/
dC
B)
dL < 1/
dC
C)
dL = 1/
dC
D)
dL > R
E)
dL < R
65. In a sinusoidally driven series RLC circuit, the inductive resistance is XL = 200 , the
capacitive reactance is XC = 100 , and the resistance is R = 50 . The current and applied emf
would be in phase if:
A) the resistance is increased to 100 , with no other changes
B) the resistance is increased to 200 , with no other changes