WorksheetsElectromagentic , Mid-term 2 , questions
Total questions: 76
Worksheet time: 25mins
In an RC circuit during charging, the voltage across the capacitor is given by:
V(t) = V0(e^(t/RC))
V(t) = V0(1 - e^(-t/RC))
V(t) = V0(1 + e^(-t/RC))
V(t) = V0(e^(-t/RC))
The time constant (τ) of an RC circuit is:
τ = R × C
τ = C / R
τ = R / C
τ = R + C
In an RL circuit, the current during transient buildup is given by:
I(t) = (V/R)(1 + e^(-Rt/L))
I(t) = (V/R)(e^(Rt/L))
I(t) = (V/R)(1 - e^(-Rt/L))
I(t) = (V/R)(e^(-Rt/L))
The time constant (τ) of an RL circuit is:
τ = LR
τ = R/L
τ = L/R
τ = L + R
The purpose of an inductor in a circuit is to:
Oppose changes in current
Oppose changes in voltage
Store energy in an electric field
Dissipate energy as heat
In an RC circuit, the voltage across the resistor during discharging is:
V_R(t) = V_0 * e^(-t/RC)
V_R(t) = V_0 * sin(t/RC)
V_R(t) = V_0 * e^(t/RC)
V_R(t) = V_0 * (1 - e^(-t/RC))
The energy stored in a capacitor is in the form of:
Electrostatic potential energy
Kinetic energy
Thermal energy
Magnetic energy
The voltage across an inductor leads the current by:
45 degrees
90 degrees
180 degrees
0 degrees
The reactance of an inductor (XL) is given by:
XL = ωL
XL = L/ω
XL = 1/ω
XL = R
The reactance of a capacitor (XC) is given by:
XC = 2πfC^2
XC = 1 / (2πfC)
XC = C / (2πf)
XC = 2πfC
In an RL circuit, the voltage across the inductor during transient buildup is:
The voltage across the inductor is constant throughout the transient.
The voltage across the inductor is zero at all times.
The voltage across the inductor increases indefinitely during the transient.
The voltage across the inductor is initially high and decreases as the current stabilizes.
The current in an RC circuit during charging is given by:
I(t) = V * e^(t/(RC))
I(t) = (V/R) * e^(t/(RC))
I(t) = (V/R) * e^(-t/(RC))
I(t) = (V/R) * (1 - e^(-t/(RC)))
The voltage across a capacitor cannot change instantaneously because:
It stores energy in a magnetic field
It stores energy in an electric field
It opposes changes in current
It dissipates energy as heat
The current through an inductor cannot change instantaneously because:
It stores energy in a magnetic field
It stores energy in an electric field
It opposes changes in voltage
It dissipates energy as heat
The unit of inductance is:
volt
ohm
henry
farad
The time constant represents the time required for the voltage or current to reach approximately:
63.2% of its final value
100% of its final value
50% of its final value
75% of its final value
In an RL circuit, the voltage across the resistor during transient buildup is given by:
V_R(t) = I(t) * R = (V_s/R)(1 - e^(-t/(L/R))) * R = V_s(1 - e^(-t/(L/R)))
V_R(t) = V_s * e^(-t/(L/R))
V_R(t) = I(t) / R = (V_s * R)(1 + e^(-t/(L/R)))
V_R(t) = V_s * e^(t/(L/R))
The total impedance of a series RL circuit is:
Z = R² + L²
Z=R−iXC
Z=R+iXL
Z=R−iXL
Explain the transient behavior of voltage and current in an RC circuit during charging and discharging. Derive the expressions for vC(t) and iC(t) during these processes.
(a)
The unit of angular frequency (ω) is:
radians/second
revolutions/second
radians/minute
degrees/second
The relationship between frequency (f) and angular frequency (ω) is:
ω = πf
ω = 2πf
f = 2πω
ω = f/2π
The general form of a sinusoidal voltage is:
V(t) = V_m * sin(ωt + φ)
V(t) = V_m * tan(ωt)
V(t) = V_m * sin(φ)
V(t) = V_m * cos(ωt + φ)
The phase angle θ in v(t)= V_m sin(ωt+θ)represents:
The amplitude of the waveform.
The initial phase shift of the waveform.
The maximum voltage of the waveform.
The frequency of the waveform.
The phasor representation of v(t)=Vm sin(ωt+30°) is:
Vm∠30°
Vm sin(ωt)
Vm∠60°
Vm∠0°
The impedance of a resistor in an AC circuit is represented by:
Z = 1/R
Z = R + jX
Z = R^2
Z = R
The impedance of a capacitor in an AC circuit is given by:
Z = R∠0°
Z = XC∠−90°
Z = −iXC
Z = jωC
In a purely resistive AC circuit, the phase angle between voltage and current is:
90 degrees
270 degrees
180 degrees
0 degrees
In a purely inductive AC circuit, the phase angle between voltage and current is:
90 degrees
45 degrees
0 degrees
180 degrees
In a purely capacitive AC circuit, the phase angle between voltage and current is:
0 degrees
90 degrees
45 degrees
180 degrees
The total impedance of a series RLC circuit is:
Z = R + X_L + X_C
Z = √(R² + (X_L - X_C)²)
Z = R² + X_L² + X_C²
Z = R / (X_L + X_C)
The condition for resonance in a series RLC circuit is:
XL > XC
XL < XC
R = L + C
XL = XC
At resonance, the impedance of a series RLC circuit is:
R
R + jX
0
2R
The resonant frequency (fr) of a series RLC circuit is given by:
fr = LC / (2π)
fr = 1 / (2πL)
fr = 1 / (2π√(LC))
fr = √(L/C)
The power factor of an AC circuit is defined as:
The power factor is defined as the square of the current.
The power factor is defined as cos(φ), where φ is the phase angle between voltage and current.
The power factor is the product of voltage and current.
The power factor is defined as the ratio of voltage to current.
The unit of apparent power is:
joules (J)
watts (W)
volt-amperes (VA)
ohms (Ω)
The unit of real power is:
Volts (V)
Amperes (A)
Ohms (Ω)
Watts (W)
The power triangle relates:
Real power, reactive power, and apparent power.
Load, source, and circuit.
Energy, power factor, and frequency.
Voltage, current, and resistance.
At resonance, the current in a series RLC circuit is:
Zero current
Constant current
Decreasing current
Maximum current
The bandwidth of a resonant circuit is defined as:
The range of frequencies around the resonant frequency where the circuit can operate effectively.
The total resistance in the circuit at resonance.
The minimum voltage required for the circuit to function.
The maximum frequency the circuit can handle without distortion.
The quality factor (Q) of a resonant circuit is given by:
Q = f_r * Δf
Q = f_r / Δf
Q = Δf / f_r
Q = f_r + Δf
In a parallel RLC circuit at resonance, the impedance is:
Maximum
0
Unpredictable
Minimum
The power factor of a purely resistive circuit is:
0.5
2
1.5
1
The power factor of a purely inductive circuit is:
-1
0
1
0.5
The power factor of a purely capacitive circuit is:
0
0.5
-1
1
The apparent power (S) in an AC circuit is given by:
S = V + I
S = V / I
S = V - I
S = V * I
The real power (P) in an AC circuit is given by:
P = VIcos(φ)
P = V^2/R
P = VIsin(φ)
P = VI
The reactive power (Q) in an AC circuit is given by:
Q = V * I * cos(φ)
Q = V / I * tan(φ)
Q = V + I * φ
Q = V * I * sin(φ)
The power factor angle (θ) is the angle between:
The voltage and the power in a DC circuit.
The voltage and the current in an AC circuit.
The frequency and the amplitude of a signal.
The resistance and the capacitance in a circuit.
A lagging power factor implies that the current:
lags behind the voltage
is independent of the voltage
leads the voltage
is in phase with the voltage
A leading power factor implies that the current:
is lagging the voltage.
is in phase with the voltage.
is independent of the voltage.
is leading the voltage.
The unit of admittance is:
The admittance (Y) of a circuit is:
The conductance (G) of a circuit is:
The susceptance (B) of a circuit is:
The admittance of a resistor is:
Y=G∠0°
Y=B∠−90°
Y=G+iB
Y=G−iB
The admittance of an inductor is:
Y=G∠0
Y=B∠−90°
Y=G+ji
Y=G−iB
The admittance of a capacitor is:
Y=G∠0°
Y=B∠90°
Y=G+iB
Y=G−iB
The unit of magnetic flux (Φ) is:
The unit of magnetic flux density (B) is:
The relationship between magnetic flux (Φ) and flux density (B) is:
The magnetomotive force (mmf) is given by
The reluctance (R) of a magnetic circuit is given by:
Ohm's law for magnetic circuits is:
The permeability of free space (μ0) is:
The relative permeability (μr) of a material is:
μr=μ/μ0
μr=μ0/μ
μr=μ+μ0
μr=μ−μ0
Ferromagnetic materials have:
The magnetizing force (H) is given by:
H=NI/j
H=Φ/A
H=B/μ
H=F/R
The relationship between B and H is:
B=μH
B=H/μ
B=μ/H
B=H+μ
Ampère's circuital law states that:
∑NI=∑Hj
∑Hj=∑NI
∑Φ=0
∑B=0
The principle of a DC motor is based on:
Faraday's law of induction
Fleming's left-hand rule
Ohm's law
Kirchhoff's law
The commutator in a DC motor is used to:
Decrease the torque
Increase the speed of the motor
Reverse the direction of current in the armature
Generate magnetic flux
The armature in a DC motor is the:
The brushes in a DC motor are used to:
The back emf in a DC motor is proportional to:
The torque produced by a DC motor is proportional to:
The speed of a DC motor can be controlled by:
Varying the voltage
None of the above
