Electricity and Magnetism

198 questions

Question 41Question

An alternating current (AC) circuit consists of a 40 Ω40\ \Omega resistor, an inductor with a reactance of 70 Ω70\ \Omega, and a capacitor with a reactance of 40 Ω40\ \Omega connected in series across an AC supply. What is the power factor of the circuit?

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Answer: 0.80

Answer

0.80
The total impedance of the series RLC circuit is found using phasor addition: Z=402+(7040)2=50 ΩZ = \sqrt{40^2 + (70 - 40)^2} = 50\ \Omega. The power factor is the ratio of resistance to impedance: cosθ=4050=0.80\cos \theta = \frac{40}{50} = 0.80.

Step-by-Step Solution

1
Calculate the net reactance (XnetX_{\text{net}}) of the circuit
Xnet=XLXC=70 Ω40 Ω=30 ΩX_{\text{net}} = X_L - X_C = 70\ \Omega - 40\ \Omega = 30\ \Omega
In a series RLC circuit, inductive and capacitive reactances oppose each other in phase.
2
Calculate total impedance (ZZ) using phasor addition
Z=R2+(XLXC)2=402+302=1600+900=50 ΩZ = \sqrt{R^2 + (X_L - X_C)^2} = \sqrt{40^2 + 30^2} = \sqrt{1600 + 900} = 50\ \Omega
Resistance and net reactance act at right angles in the impedance phasor diagram.
3
Calculate the power factor (cosθ\cos \theta)
cosθ=RZ=4050=0.80\cos \theta = \frac{R}{Z} = \frac{40}{50} = 0.80
The power factor is defined as the cosine of the phase angle, which equals the ratio of resistance to total impedance.

Key Concept

Power factor of a series RLC AC circuit
Estimated Time:1m 30s
Question 42Question

A series alternating current (AC) circuit contains an inductor of inductance L=1π2 HL = \frac{1}{\pi^2}\ \text{H}, a capacitor of capacitance C=25 μFC = 25\ \mu\text{F}, and a resistor of resistance R=50 ΩR = 50\ \Omega. What is the resonant frequency of the circuit in hertz (Hz\text{Hz})?

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Answer: 100

Answer

The resonant frequency of the circuit is 100 Hz100\ \text{Hz}.
At resonance, the inductive reactance XL=2πfLX_L = 2\pi f L equals the capacitive reactance XC=12πfCX_C = \frac{1}{2\pi f C}. Equating both yields f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}. Substituting L=1π2 HL = \frac{1}{\pi^2}\ \text{H} and C=25×106 FC = 25 \times 10^{-6}\ \text{F} gives LC=5×103π s\sqrt{LC} = \frac{5 \times 10^{-3}}{\pi}\ \text{s}, leading to f0=12π(5×103π)=100 Hzf_0 = \frac{1}{2\pi \left(\frac{5 \times 10^{-3}}{\pi}\right)} = 100\ \text{Hz}.

Step-by-Step Solution

1
Write down the formula for the resonant frequency of a series RLC circuit.
f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}
Resonance occurs when the inductive reactance equals the capacitive reactance (XL=XCX_L = X_C).
2
Substitute the values of inductance L=1π2 HL = \frac{1}{\pi^2}\ \text{H} and capacitance C=25×106 FC = 25 \times 10^{-6}\ \text{F} into LC\sqrt{LC}.
LC=1π2×25×106=5×103π s\sqrt{LC} = \sqrt{\frac{1}{\pi^2} \times 25 \times 10^{-6}} = \frac{5 \times 10^{-3}}{\pi}\ \text{s}
Simplifying the square root removes the fraction containing π\pi.
3
Calculate the resonant frequency f0f_0.
f0=12π×5×103π=1102=100 Hzf_0 = \frac{1}{2\pi \times \frac{5 \times 10^{-3}}{\pi}} = \frac{1}{10^{-2}} = 100\ \text{Hz}
The factor of π\pi cancels out in the denominator, resulting in a whole number value.

Key Concept

Resonant Frequency in AC Series Circuits
Estimated Time:1m 30s
Question 43Question

At a point on the Earth's surface, the total magnetic intensity is 4.0×105 T4.0 \times 10^{-5}\text{ T} and the angle of dip is 6060^\circ. What is the horizontal component of the Earth's magnetic field at this point?

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Answer: 2.0×105 T2.0 \times 10^{-5}\text{ T}

Answer

The horizontal component of the Earth's magnetic field is 2.0×105 T2.0 \times 10^{-5}\text{ T}.
The horizontal component BhB_h of the Earth's magnetic field is given by resolving the total magnetic intensity BB along the horizontal direction using Bh=BcosθB_h = B \cos \theta. Substituting B=4.0×105 TB = 4.0 \times 10^{-5}\text{ T} and θ=60\theta = 60^\circ yields Bh=4.0×105×0.5=2.0×105 TB_h = 4.0 \times 10^{-5} \times 0.5 = 2.0 \times 10^{-5}\text{ T}.

Step-by-Step Solution

1
Identify the given values and formula
Total field B=4.0×105 TB = 4.0 \times 10^{-5}\text{ T}, Angle of dip θ=60\theta = 60^\circ. Formula: Bh=BcosθB_h = B \cos \theta
The horizontal component of Earth's magnetic field is obtained by resolving the total magnetic vector along the horizontal plane.
2
Substitute the given values into the equation
Bh=4.0×105 T×cos(60)=4.0×105×0.5=2.0×105 TB_h = 4.0 \times 10^{-5}\text{ T} \times \cos(60^\circ) = 4.0 \times 10^{-5} \times 0.5 = 2.0 \times 10^{-5}\text{ T}
Since cos(60)=0.5\cos(60^\circ) = 0.5, evaluating the product gives the exact horizontal component.

Key Concept

Resolution of Earth's Magnetic Field Components
Question 44Question

A galvanometer with an internal resistance of 5 Ω5\text{ }\Omega produces a full-scale deflection when a current of 10 mA10\text{ mA} flows through it. Calculate the shunt resistance, in ohms, required to convert this galvanometer into an ammeter capable of measuring currents up to 50 mA50\text{ mA}.

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Answer: 1.25

Answer

The required shunt resistance is 1.25 Ω1.25\text{ }\Omega.
To extend the range of a galvanometer, a shunt resistor SS is placed in parallel with it. The potential difference across the galvanometer equals the potential difference across the shunt: IgRg=(IIg)SI_g R_g = (I - I_g) S. Substituting the given values Rg=5 ΩR_g = 5\text{ }\Omega, Ig=10 mAI_g = 10\text{ mA}, and maximum current I=50 mAI = 50\text{ mA} yields 10 mA×5 Ω=(50 mA10 mA)×S10\text{ mA} \times 5\text{ }\Omega = (50\text{ mA} - 10\text{ mA}) \times S, solving to S=5040=1.25 ΩS = \frac{50}{40} = 1.25\text{ }\Omega.

Step-by-Step Solution

1
Find the current passing through the parallel shunt resistor
Is=40 mAI_s = 40\text{ mA}
By Kirchhoff's current law, the total maximum current divides into the galvanometer current and the shunt current (I=Ig+IsI = I_g + I_s).
2
Calculate the required shunt resistance SS
S=1.25 ΩS = 1.25\text{ }\Omega
Because the galvanometer and shunt resistor are connected in parallel, the potential difference across both branches is equal (IgRg=IsSI_g R_g = I_s S).

Key Concept

Conversion of a galvanometer to an ammeter using a low-resistance shunt in parallel
Question 45Question

Match each electrical quantity or operational scenario on the left with its corresponding mathematical expression on the right.

Click a left item, then click its matching right item

Items

Electrical power dissipated in a resistor of resistance RR carrying current II
Electrical energy consumed by a device of resistance RR operating across potential difference VV for duration tt
Rate of heat generation in a component operating with potential difference VV and current II
Total electric charge transferred across a potential difference VV when electrical energy EE is transformed

Matches

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Answer

Electrical power in terms of current and resistance corresponds to I2RI^2 R. Electrical energy consumed across voltage VV for time tt corresponds to V2tR\frac{V^2 t}{R}. Rate of heat generation in terms of voltage and current corresponds to VIV I. Total electric charge transformed corresponds to EV\frac{E}{V}.
Each item is matched by applying the fundamental relationships of electrical energy (E=VIt=I2Rt=V2tR=QVE = V I t = I^2 R t = \frac{V^2 t}{R} = Q V) and electrical power (P=Et=VI=I2R=V2RP = \frac{E}{t} = V I = I^2 R = \frac{V^2}{R}).

Step-by-Step Solution

1
Analyze the first scenario (power with current and resistance)
Power formula derived from Ohm's law (V=IRV = IR) into P=VIP = VI gives P=(IR)I=I2RP = (IR)I = I^2 R.
Relates current and resistance directly to power dissipation.
2
Analyze the second scenario (energy with voltage, resistance, and time)
Energy E=PtE = P t. Using P=V2RP = \frac{V^2}{R}, energy becomes E=V2tRE = \frac{V^2 t}{R}.
Expresses energy consumption using voltage and resistance over a given time duration.
3
Analyze the third scenario (rate of heat generation with voltage and current)
Rate of heat generation is power P=VIP = V I.
Direct definition of electrical power as energy converted per unit time.
4
Analyze the fourth scenario (charge transferred from energy and voltage)
Since potential difference is energy per unit charge (V=EQV = \frac{E}{Q}), rearranging gives Q=EVQ = \frac{E}{V}.
Relates fundamental definitions of potential difference, energy, and charge.

Key Concept

Formulas for Electrical Energy, Power, and Charge
Question 46Question

A point charge of +5.0×108 C+5.0 \times 10^{-8}\text{ C} is situated in a vacuum. Taking Coulomb's constant k=9.0×109 Nm2C2k = 9.0 \times 10^9\text{ N}\cdot\text{m}^2\text{C}^{-2}, what is the magnitude of the electric field intensity, in N C1\text{N C}^{-1}, at a distance of 0.3 m0.3\text{ m} from the charge?

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Answer: 5000

Answer

The magnitude of the electric field intensity at a distance of 0.3 m0.3\text{ m} is 5000 N C15000\text{ N C}^{-1}.
The electric field intensity EE at a distance rr from a point charge qq in free space is given by E=kqr2E = \frac{k |q|}{r^2}. Substituting k=9.0×109 Nm2C2k = 9.0 \times 10^9\text{ N}\cdot\text{m}^2\text{C}^{-2}, q=5.0×108 Cq = 5.0 \times 10^{-8}\text{ C}, and r=0.3 mr = 0.3\text{ m} into the expression yields E=9.0×109×5.0×108(0.3)2=4500.09=5000 N C1E = \frac{9.0 \times 10^9 \times 5.0 \times 10^{-8}}{(0.3)^2} = \frac{450}{0.09} = 5000\text{ N C}^{-1}.

Step-by-Step Solution

1
Identify the given values and formula
q=5.0×108 Cq = 5.0 \times 10^{-8}\text{ C}, r=0.3 mr = 0.3\text{ m}, k=9.0×109 Nm2C2k = 9.0 \times 10^9\text{ N}\cdot\text{m}^2\text{C}^{-2}, and E=kqr2E = \frac{k |q|}{r^2}
Electric field intensity surrounding a point charge depends on the charge magnitude and inversely on the square of the distance.
2
Calculate the square of the distance
r2=(0.3)2=0.09 m2r^2 = (0.3)^2 = 0.09\text{ m}^2
The inverse-square law requires using r2r^2 in the denominator.
3
Substitute values and solve for field intensity
E=9.0×109×5.0×1080.09=4500.09=5000 N C1E = \frac{9.0 \times 10^9 \times 5.0 \times 10^{-8}}{0.09} = \frac{450}{0.09} = 5000\text{ N C}^{-1}
Multiplying the terms in the numerator yields 450 Nm2C1450\text{ N}\cdot\text{m}^2\text{C}^{-1}, and dividing by 0.09 m20.09\text{ m}^2 gives 5000 N C15000\text{ N C}^{-1}.

Key Concept

Electric field intensity due to a isolated point charge
Question 47Question

Two identical insulated conducting spheres, XX and YY, carry initial charges of +8.0×109 C+8.0 \times 10^{-9}\text{ C} and 2.0×109 C-2.0 \times 10^{-9}\text{ C}, respectively. They are brought into brief contact and then separated by a distance of 0.3 m0.3\text{ m} in a vacuum. Taking Coulomb's constant k=9.0×109 Nm2C2k = 9.0 \times 10^9\text{ N}\cdot\text{m}^2\text{C}^{-2}, what is the magnitude of the electrostatic force between the two spheres after separation?

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Answer: 9.0×107 N9.0 \times 10^{-7}\text{ N}

Answer

The magnitude of the electrostatic force between the spheres after separation is 9.0×107 N9.0 \times 10^{-7}\text{ N}.
When two identical conducting spheres touch, the total charge conserves and divides equally between them. The net charge is (+8.0×109 C)+(2.0×109 C)=+6.0×109 C(+8.0 \times 10^{-9}\text{ C}) + (-2.0 \times 10^{-9}\text{ C}) = +6.0 \times 10^{-9}\text{ C}, yielding +3.0×109 C+3.0 \times 10^{-9}\text{ C} on each sphere. Substituting these equal charges and distance 0.3 m0.3\text{ m} into Coulomb's law gives F=9.0×109×(3.0×109)20.09=9.0×107 NF = \frac{9.0 \times 10^9 \times (3.0 \times 10^{-9})^2}{0.09} = 9.0 \times 10^{-7}\text{ N}.

Step-by-Step Solution

1
Calculate the total net charge after contact and the charge on each identical sphere.
Net charge Qnet=(+8.0×109 C)+(2.0×109 C)=+6.0×109 CQ_{net} = (+8.0 \times 10^{-9}\text{ C}) + (-2.0 \times 10^{-9}\text{ C}) = +6.0 \times 10^{-9}\text{ C}. Since the spheres are identical, the charge on each sphere is q=+6.0×109 C2=+3.0×109 Cq = \frac{+6.0 \times 10^{-9}\text{ C}}{2} = +3.0 \times 10^{-9}\text{ C}.
When identical conductors touch, total charge is conserved and redistributes equally between them.
2
Apply Coulomb's Law using the redistributed charge and separation distance.
F=kq1q2r2=(9.0×109)(3.0×109)(3.0×109)(0.3)2=8.1×1070.09=9.0×107 NF = k \frac{q_1 q_2}{r^2} = (9.0 \times 10^9) \frac{(3.0 \times 10^{-9})(3.0 \times 10^{-9})}{(0.3)^2} = \frac{8.1 \times 10^{-7}}{0.09} = 9.0 \times 10^{-7}\text{ N}.
Coulomb's Law calculates the magnitude of electrostatic force between two point-like charges at a given distance.

Key Concept

Charge conservation, redistribution between identical conductors, and Coulomb's Law
Estimated Time:1m 30s
Question 48Question

A point charge of +6.0×106 C+6.0 \times 10^{-6}\text{ C} experiences an attractive electrostatic force of 0.54 N0.54\text{ N} when placed at a distance of 1.0 m1.0\text{ m} from a second point charge in a vacuum. Taking Coulomb's constant k=9.0×109 Nm2C2k = 9.0 \times 10^9\text{ N}\cdot\text{m}^2\text{C}^{-2}, what is the magnitude of the second charge in microcoulombs (μC\mu\text{C})?

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Answer: 10

Answer

The magnitude of the second charge is 10 µC.
Using Coulomb's law F=kq1q2r2F = \frac{k |q_1 q_2|}{r^2}, substituting F=0.54 NF = 0.54\text{ N}, q1=6.0×106 Cq_1 = 6.0 \times 10^{-6}\text{ C}, r=1.0 mr = 1.0\text{ m}, and k=9.0×109 Nm2C2k = 9.0 \times 10^9\text{ N}\cdot\text{m}^2\text{C}^{-2} yields q2=1.0×105 C|q_2| = 1.0 \times 10^{-5}\text{ C}, which equals 10 μC10\text{ }\mu\text{C}.

Step-by-Step Solution

1
State Coulomb's Law formula
F=kq1q2r2F = \frac{k |q_1 q_2|}{r^2}
Coulomb's Law describes the electrostatic force between two point charges.
2
Substitute given parameters into the equation
0.54=9.0×109×6.0×106×q21.020.54 = \frac{9.0 \times 10^9 \times 6.0 \times 10^{-6} \times |q_2|}{1.0^2}
Knowns: F=0.54 NF = 0.54\text{ N}, q1=6.0×106 Cq_1 = 6.0 \times 10^{-6}\text{ C}, r=1.0 mr = 1.0\text{ m}, k=9.0×109 Nm2C2k = 9.0 \times 10^9\text{ N}\cdot\text{m}^2\text{C}^{-2}.
3
Solve for the unknown charge magnitude q2q_2
q2=1.0×105 C|q_2| = 1.0 \times 10^{-5}\text{ C}
Rearranging yields q2=0.545.4×104=1.0×105 C|q_2| = \frac{0.54}{5.4 \times 10^4} = 1.0 \times 10^{-5}\text{ C}.
4
Convert the value from Coulombs to microcoulombs
10 μC10\text{ }\mu\text{C}
1 μC=106 C1\text{ }\mu\text{C} = 10^{-6}\text{ C}, so 1.0×105 C=10 μC1.0 \times 10^{-5}\text{ C} = 10\text{ }\mu\text{C}.

Key Concept

Coulomb's Law
Question 49Question

Two capacitors with capacitances of 3 μF3\text{ }\mu\text{F} and 6 μF6\text{ }\mu\text{F} are connected in parallel. This combination is then connected in series with a 9 μF9\text{ }\mu\text{F} capacitor across a 12 V12\text{ }\text{V} direct current source. What is the total electrical energy stored in the network?

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Answer: 3.24×104 J3.24 \times 10^{-4}\text{ }\text{J}

Answer

The total electrical energy stored in the network is 3.24×104 J3.24 \times 10^{-4}\text{ }\text{J}.
First, find the equivalent capacitance of the parallel branch (3 μF+6 μF=9 μF3\text{ }\mu\text{F} + 6\text{ }\mu\text{F} = 9\text{ }\mu\text{F}). Next, combine this with the 9 μF9\text{ }\mu\text{F} capacitor in series, yielding Ceq=9×99+9=4.5 μF=4.5×106 FC_{eq} = \frac{9 \times 9}{9 + 9} = 4.5\text{ }\mu\text{F} = 4.5 \times 10^{-6}\text{ }\text{F}. Finally, substituting into the stored energy formula E=12CeqV2E = \frac{1}{2} C_{eq} V^2 gives E=0.5×4.5×106×144=3.24×104 JE = 0.5 \times 4.5 \times 10^{-6} \times 144 = 3.24 \times 10^{-4}\text{ }\text{J}.

Step-by-Step Solution

1
Calculate equivalent capacitance of the parallel section
Cp=C1+C2=3 μF+6 μF=9 μFC_p = C_1 + C_2 = 3\text{ }\mu\text{F} + 6\text{ }\mu\text{F} = 9\text{ }\mu\text{F}
Capacitors in parallel add directly.
2
Calculate total equivalent capacitance of the network
1Ceq=1Cp+1C3=19 μF+19 μF=29 μF    Ceq=4.5 μF=4.5×106 F\frac{1}{C_{eq}} = \frac{1}{C_p} + \frac{1}{C_3} = \frac{1}{9\text{ }\mu\text{F}} + \frac{1}{9\text{ }\mu\text{F}} = \frac{2}{9\text{ }\mu\text{F}} \implies C_{eq} = 4.5\text{ }\mu\text{F} = 4.5 \times 10^{-6}\text{ }\text{F}
Capacitors in series combine via reciprocals.
3
Calculate total stored electrical energy
E=12CeqV2=12×(4.5×106 F)×(12 V)2=3.24×104 JE = \frac{1}{2} C_{eq} V^2 = \frac{1}{2} \times (4.5 \times 10^{-6}\text{ }\text{F}) \times (12\text{ }\text{V})^2 = 3.24 \times 10^{-4}\text{ }\text{J}
Energy stored in a capacitor network depends on equivalent capacitance and potential difference across it.

Key Concept

Equivalent capacitance of series-parallel combinations and energy stored in a capacitor
Question 50Question

A parallel plate capacitor with a capacitance of 12 μF12\text{ }\mu\text{F} is fully charged by connecting it across a 50 V50\text{ V} direct current power source. What is the total electrostatic energy stored in the capacitor in millijoules (mJ\text{mJ})?

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Answer: 15

Answer

The total electrostatic energy stored in the capacitor is 15 mJ15\text{ mJ}.
The energy stored in a capacitor is given by E=12CV2E = \frac{1}{2}CV^2. Substituting C=12×106 FC = 12 \times 10^{-6}\text{ F} and V=50 VV = 50\text{ V} yields E=12×12×106×2500=0.015 J=15 mJE = \frac{1}{2} \times 12 \times 10^{-6} \times 2500 = 0.015\text{ J} = 15\text{ mJ}.

Step-by-Step Solution

1
Convert given values to standard SI units.
C=12×106 FC = 12 \times 10^{-6}\text{ F}, V=50 VV = 50\text{ V}
Calculating in SI units ensures the resultant energy is in Joules.
2
Apply the formula for energy stored in a charged capacitor.
E=12CV2E = \frac{1}{2} C V^2
Work done during charging is stored as electrostatic potential energy in the electric field between the plates.
3
Substitute the values and convert Joules to millijoules.
E=12×(12×106)×2500=0.015 J=15 mJE = \frac{1}{2} \times (12 \times 10^{-6}) \times 2500 = 0.015\text{ J} = 15\text{ mJ}
Multiplying Joules by 10310^3 converts the result into millijoules.

Key Concept

Energy stored in a capacitor (E=12CV2E = \frac{1}{2}CV^2)
Question 51Question

A capacitor of capacitance 5 μF5\text{ }\mu\text{F} is charged to a potential difference of 200 V200\text{ V} and then disconnected from the power supply. If it is subsequently connected in parallel across an uncharged capacitor of capacitance 15 μF15\text{ }\mu\text{F}, what is the final common potential difference across the combination in volts?

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Answer: 50

Answer

The final common potential difference across the combination is 50 V.
By charge conservation, the total charge Q=C1V1=5 μF×200 V=1000 μCQ = C_1 V_1 = 5\text{ }\mu\text{F} \times 200\text{ V} = 1000\text{ }\mu\text{C} is shared across the two parallel capacitors. The total equivalent capacitance is Ctotal=C1+C2=20 μFC_{\text{total}} = C_1 + C_2 = 20\text{ }\mu\text{F}. Therefore, the final potential difference is V=QCtotal=1000 μC20 μF=50 VV = \frac{Q}{C_{\text{total}}} = \frac{1000\text{ }\mu\text{C}}{20\text{ }\mu\text{F}} = 50\text{ V}.

Step-by-Step Solution

1
Calculate the initial electric charge (QQ) stored on the charged capacitor
Q=5 μF×200 V=1000 μCQ = 5\text{ }\mu\text{F} \times 200\text{ V} = 1000\text{ }\mu\text{C}
Before connection, all charge is stored solely on the 5 μF5\text{ }\mu\text{F} capacitor.
2
Calculate the total equivalent capacitance (CtotalC_{\text{total}}) of the parallel network
Ctotal=5 μF+15 μF=20 μFC_{\text{total}} = 5\text{ }\mu\text{F} + 15\text{ }\mu\text{F} = 20\text{ }\mu\text{F}
Capacitors in parallel add directly (Ctotal=C1+C2C_{\text{total}} = C_1 + C_2).
3
Apply the law of conservation of charge to find the final common voltage (VV)
V=QCtotal=1000 μC20 μF=50 VV = \frac{Q}{C_{\text{total}}} = \frac{1000\text{ }\mu\text{C}}{20\text{ }\mu\text{F}} = 50\text{ V}
The total charge remains conserved and redistributes across the total combined capacitance.

Key Concept

Charge Redistribution and Conservation in Parallel Capacitors
Question 52Question

An electric heating element made of a wire with resistivity 1.0×106Ωm1.0 \times 10^{-6}\,\Omega\cdot\text{m} and a uniform cross-sectional area of 5.0×107m25.0 \times 10^{-7}\,\text{m}^2 carries a steady current of 4.0A4.0\,\text{A} when connected to a 240V240\,\text{V} direct-current supply. What is the length of the wire?

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Answer: 30m30\,\text{m}

Answer

30m30\,\text{m}
By applying Ohm's Law (R=VIR = \frac{V}{I}), the total resistance of the heating element is found to be 60Ω60\,\Omega. Substituting this along with resistivity ρ=1.0×106Ωm\rho = 1.0 \times 10^{-6}\,\Omega\cdot\text{m} and cross-sectional area A=5.0×107m2A = 5.0 \times 10^{-7}\,\text{m}^2 into the resistivity equation R=ρLAR = \frac{\rho L}{A} yields L=RAρ=30mL = \frac{R A}{\rho} = 30\,\text{m}.

Step-by-Step Solution

1
Calculate the electrical resistance of the wire using Ohm's Law.
R=VI=240V4.0A=60ΩR = \frac{V}{I} = \frac{240\,\text{V}}{4.0\,\text{A}} = 60\,\Omega
The resistance must be determined from the operational potential difference and current before finding the geometric dimensions.
2
Relate resistance to length, cross-sectional area, and resistivity using R=ρLAR = \frac{\rho L}{A}.
60Ω=(1.0×106Ωm)×L5.0×107m260\,\Omega = \frac{(1.0 \times 10^{-6}\,\Omega\cdot\text{m}) \times L}{5.0 \times 10^{-7}\,\text{m}^2}
The resistance of a uniform conductor is directly proportional to its length and inversely proportional to its cross-sectional area.
3
Solve the equation for the wire length LL.
L=60×5.0×1071.0×106=30mL = \frac{60 \times 5.0 \times 10^{-7}}{1.0 \times 10^{-6}} = 30\,\text{m}
Rearranging the formula gives L=RAρL = \frac{R A}{\rho} to isolate the required length.

Key Concept

Relationship between potential difference, current, resistance, and wire dimensions (R=VI=ρLAR = \frac{V}{I} = \frac{\rho L}{A})
Question 53Question

A galvanometer has an internal resistance of 20 Ω20\text{ }\Omega and produces a full-scale deflection for a current of 15 mA15\text{ mA}. What resistance of the multiplier, in ohms (Ω\Omega), is required to convert this galvanometer into a voltmeter capable of measuring a maximum potential difference of 30 V30\text{ V}?

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Answer: 1980

Answer

The required multiplier resistance is 1980 Ω1980\text{ }\Omega.
To convert a galvanometer into a voltmeter, a multiplier resistor RmR_m is connected in series. The maximum potential difference VV across the combination is given by V=Ig(Rg+Rm)V = I_g(R_g + R_m). Substituting V=30 VV = 30\text{ V}, Ig=0.015 AI_g = 0.015\text{ A}, and Rg=20 ΩR_g = 20\text{ }\Omega yields Rm=1980 ΩR_m = 1980\text{ }\Omega.

Step-by-Step Solution

1
Convert current from milliamperes to amperes.
Ig=15 mA=0.015 AI_g = 15\text{ mA} = 0.015\text{ A}.
Standard electrical formulas require current in amperes.
2
Apply the relationship between voltage range, galvanometer current, internal resistance, and multiplier resistance.
V=Ig(Rg+Rm)V = I_g(R_g + R_m), where V=30 VV = 30\text{ V}, Ig=0.015 AI_g = 0.015\text{ A}, and Rg=20 ΩR_g = 20\text{ }\Omega.
A multiplier resistor is connected in series with the galvanometer so that the total potential difference is distributed across both components.
3
Rearrange the equation and compute RmR_m.
Rm=300.01520=200020=1980 ΩR_m = \frac{30}{0.015} - 20 = 2000 - 20 = 1980\text{ }\Omega.
Subtracting the internal resistance of the galvanometer from the total required resistance yields the necessary multiplier resistance.

Key Concept

Galvanometer conversion to a voltmeter using a series multiplier resistor
Estimated Time:1m 30s
Question 54Question

A resistance thermometer has a resistance of 5.0Ω5.0\,\Omega at 0C0^\circ\text{C} and 5.8Ω5.8\,\Omega at 40C40^\circ\text{C}. What is the temperature coefficient of resistance of the material in K1\text{K}^{-1}?

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Answer: 0.004

Answer

The temperature coefficient of resistance of the material is 0.004K10.004\,\text{K}^{-1} (or 4.0×103K14.0 \times 10^{-3}\,\text{K}^{-1}).
The temperature coefficient of resistance is calculated using α=RTR0R0ΔT\alpha = \frac{R_T - R_0}{R_0 \Delta T}. Substituting R0=5.0ΩR_0 = 5.0\,\Omega, RT=5.8ΩR_T = 5.8\,\Omega, and ΔT=40K\Delta T = 40\,\text{K} yields α=0.8200=0.004K1\alpha = \frac{0.8}{200} = 0.004\,\text{K}^{-1}.

Step-by-Step Solution

1
Identify the relationship between resistance and temperature.
RT=R0(1+αΔT)R_T = R_0(1 + \alpha \Delta T), with R0=5.0ΩR_0 = 5.0\,\Omega, RT=5.8ΩR_T = 5.8\,\Omega, and ΔT=40C\Delta T = 40^\circ\text{C}.
The resistance of metallic conductors varies linearly with temperature for moderate temperature changes.
2
Rearrange the expression to isolate the temperature coefficient α\alpha.
\alpha = \frac{R_T - R_0}{R_0 \Delta T}
Isolating α\alpha allows direct computation from the given resistance values and temperature interval.
3
Calculate the numerical value of α\alpha.
\alpha = \frac{5.8 - 5.0}{5.0 \times 40} = \frac{0.8}{200} = 0.004\,\text{K}^{-1}
Dividing the change in resistance by the product of initial resistance and temperature change gives the fractional resistance change per unit temperature change.

Key Concept

Temperature dependence of electrical resistance and temperature coefficient of resistance.
Question 55Question

A uniform cylindrical wire of length 2.0m2.0\,\text{m} and radius 1.0mm1.0\,\text{mm} is connected to a direct-current source. When a potential difference of 12V12\,\text{V} is applied across its ends, a steady current of 4.0A4.0\,\text{A} flows through it. Taking π3.142\pi \approx 3.142, what is the resistivity of the material of the wire?

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Answer: 4.71×106Ωm4.71 \times 10^{-6}\,\Omega\cdot\text{m}

Answer

The resistivity of the material of the wire is 4.71×106Ωm4.71 \times 10^{-6}\,\Omega\cdot\text{m}.
Using Ohm's law (R=V/IR = V/I), the wire's resistance is 3.0Ω3.0\,\Omega. Substituting this resistance, the wire length (2.0m2.0\,\text{m}), and the circular area (A=πr2=3.142×106m2A = \pi r^2 = 3.142 \times 10^{-6}\,\text{m}^2) into ρ=RA/L\rho = R A / L yields 4.71×106Ωm4.71 \times 10^{-6}\,\Omega\cdot\text{m}.

Step-by-Step Solution

1
Calculate the resistance of the wire using Ohm's Law.
R=VI=12V4.0A=3.0ΩR = \frac{V}{I} = \frac{12\,\text{V}}{4.0\,\text{A}} = 3.0\,\Omega
Ohm's Law relates potential difference, current, and resistance.
2
Calculate the cross-sectional area of the wire from its radius.
A=πr2=3.142×(1.0×103m)2=3.142×106m2A = \pi r^2 = 3.142 \times (1.0 \times 10^{-3}\,\text{m})^2 = 3.142 \times 10^{-6}\,\text{m}^2
The wire has a circular cross-section.
3
Rearrange the resistance formula R=ρLAR = \frac{\rho L}{A} to solve for resistivity ρ\rho.
ρ=RAL=3.0Ω×3.142×106m22.0m=4.713×106Ωm4.71×106Ωm\rho = \frac{R A}{L} = \frac{3.0\,\Omega \times 3.142 \times 10^{-6}\,\text{m}^2}{2.0\,\text{m}} = 4.713 \times 10^{-6}\,\Omega\cdot\text{m} \approx 4.71 \times 10^{-6}\,\Omega\cdot\text{m}
Resistivity is an intrinsic property derived from resistance, length, and cross-sectional area.

Key Concept

Relationship between resistance, potential difference, current, and material resistivity.
Question 56Question

A potential difference of 16V16\,\text{V} is applied across a uniform conductor of length 4.0m4.0\,\text{m} and cross-sectional area 1.5×106m21.5 \times 10^{-6}\,\text{m}^2. If the resistivity of the conductor material is 3.0×107Ωm3.0 \times 10^{-7}\,\Omega\cdot\text{m}, what is the electric current, in amperes, flowing through the conductor?

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Answer: 20

Answer

The electric current flowing through the conductor is 20A20\,\text{A}.
The electrical resistance of the wire is first determined using the formula R=ρLA=(3.0×107)(4.0)1.5×106=0.8ΩR = \frac{\rho L}{A} = \frac{(3.0 \times 10^{-7})(4.0)}{1.5 \times 10^{-6}} = 0.8\,\Omega. Then, by applying Ohm's law (I=VRI = \frac{V}{R}), the current is computed as I=160.8=20AI = \frac{16}{0.8} = 20\,\text{A}.

Step-by-Step Solution

1
Calculate the electrical resistance of the conductor from its physical dimensions and resistivity.
R=0.8ΩR = 0.8\,\Omega
Substitute ρ=3.0×107Ωm\rho = 3.0 \times 10^{-7}\,\Omega\cdot\text{m}, L=4.0mL = 4.0\,\text{m}, and A=1.5×106m2A = 1.5 \times 10^{-6}\,\text{m}^2 into R=ρLAR = \frac{\rho L}{A}.
2
Apply Ohm's law to calculate the current flowing through the conductor.
I=20AI = 20\,\text{A}
Substitute potential difference V=16VV = 16\,\text{V} and calculated resistance R=0.8ΩR = 0.8\,\Omega into I=VRI = \frac{V}{R}.

Key Concept

Relationship between resistivity, resistance, potential difference, and electric current
Question 57Question

A steady electric current of 3.2A3.2\,\text{A} flows through a conductor for 5.0minutes5.0\,\text{minutes}. Given that the elementary charge is 1.6×1019C1.6 \times 10^{-19}\,\text{C}, how many electrons pass through a cross-section of the conductor during this period?

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Answer: 6.0×10216.0 \times 10^{21}

Answer

The number of electrons passing through the cross-section of the conductor is 6.0×10216.0 \times 10^{21}.
Electric current II is related to total electric charge QQ and time tt by Q=I×tQ = I \times t. Converting time into seconds gives t=5.0×60=300st = 5.0 \times 60 = 300\,\text{s}. The total charge passed is Q=3.2A×300s=960CQ = 3.2\,\text{A} \times 300\,\text{s} = 960\,\text{C}. Using the charge quantization formula Q=neQ = n \cdot e, the number of electrons nn is given by n=960C1.6×1019C=6.0×1021n = \frac{960\,\text{C}}{1.6 \times 10^{-19}\,\text{C}} = 6.0 \times 10^{21}.

Step-by-Step Solution

1
Convert the time from minutes into seconds.
t=5.0minutes=5.0×60s=300st = 5.0\,\text{minutes} = 5.0 \times 60\,\text{s} = 300\,\text{s}
SI units require time to be in seconds when calculating electric charge.
2
Calculate the total electric charge passing through the conductor.
Q=I×t=3.2A×300s=960CQ = I \times t = 3.2\,\text{A} \times 300\,\text{s} = 960\,\text{C}
Electric current is defined as the rate of flow of charge (I=Q/tI = Q/t).
3
Determine the number of electrons using charge quantization.
n=Qe=960C1.6×1019C=6.0×1021n = \frac{Q}{e} = \frac{960\,\text{C}}{1.6 \times 10^{-19}\,\text{C}} = 6.0 \times 10^{21}
Total charge is equal to the number of carrier electrons multiplied by the elementary charge (Q=neQ = n \cdot e).

Key Concept

Quantization of Electric Charge and Current
Question 58Question

A cell supplies a current of 0.6 A0.6\text{ A} when connected across a 2.0 Ω2.0\text{ }\Omega resistor. When the resistor is replaced with a 5.0 Ω5.0\text{ }\Omega resistor, the current supplied by the cell drops to 0.3 A0.3\text{ A}. What is the internal resistance of the cell?

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Answer: 1.0 Ω1.0\text{ }\Omega

Answer

The internal resistance of the cell is 1.0 Ω1.0\text{ }\Omega.
The electromotive force (e.m.f.) EE of a cell is given by E=I(R+r)E = I(R + r), where II is the current, RR is external resistance, and rr is internal resistance. Setting up equations for both cases: E=0.6(2.0+r)E = 0.6(2.0 + r) and E=0.3(5.0+r)E = 0.3(5.0 + r). Equating them gives 1.2+0.6r=1.5+0.3r1.2 + 0.6r = 1.5 + 0.3r, which simplifies to 0.3r=0.30.3r = 0.3, yielding r=1.0 Ωr = 1.0\text{ }\Omega.

Step-by-Step Solution

1
Formulate the electromotive force equation for the first circuit setup
E=I1(R1+r)=0.6(2.0+r)=1.2+0.6rE = I_1(R_1 + r) = 0.6(2.0 + r) = 1.2 + 0.6r
The total voltage supplied by the cell equals the total current multiplied by the sum of external and internal resistance.
2
Formulate the electromotive force equation for the second circuit setup
E=I2(R2+r)=0.3(5.0+r)=1.5+0.3rE = I_2(R_2 + r) = 0.3(5.0 + r) = 1.5 + 0.3r
The cell's electromotive force EE and internal resistance rr remain unchanged despite changing the external resistor.
3
Equate both expressions for electromotive force and solve for internal resistance
1.2+0.6r=1.5+0.3r    0.3r=0.3    r=1.0 Ω1.2 + 0.6r = 1.5 + 0.3r \implies 0.3r = 0.3 \implies r = 1.0\text{ }\Omega
Equating the two expressions allows direct solution for the single unknown variable rr.

Key Concept

Electromotive Force and Internal Resistance of Cells
Question 59Question

In a metre bridge experiment, a standard resistor of 4.0 Ω4.0\text{ }\Omega is connected in the left gap and an unknown resistor RR is connected in the right gap. When balanced, the balance point is found at a distance of 40.0 cm40.0\text{ cm} from the left end of the 100.0 cm100.0\text{ cm} bridge wire. What is the value of the unknown resistance RR in ohms?

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Answer: 6

Answer

The value of the unknown resistance RR is 6.0 Ω6.0\text{ }\Omega.
The metre bridge operates on the Wheatstone bridge principle. At balance, the ratio of the resistance in the left gap to the length of the left segment equals the ratio of the resistance in the right gap to the length of the right segment. Substituting 4.0 Ω4.0\text{ }\Omega for the left gap and 40.0 cm40.0\text{ cm} and 60.0 cm60.0\text{ cm} for the two wire lengths yields R=6.0 ΩR = 6.0\text{ }\Omega.

Step-by-Step Solution

1
Determine the length of the wire segment corresponding to the right gap.
l2=100.0 cm40.0 cm=60.0 cml_2 = 100.0\text{ cm} - 40.0\text{ cm} = 60.0\text{ cm}.
The total length of a standard metre bridge wire is 100.0 cm100.0\text{ cm}.
2
Apply the Wheatstone bridge principle for the metre bridge balance condition.
Rleftl1=Rl2    R=Rleft×l2l1\frac{R_{\text{left}}}{l_1} = \frac{R}{l_2} \implies R = R_{\text{left}} \times \frac{l_2}{l_1}.
At balance, the potential drop per unit length across the two wire segments is proportional to their respective lengths.
3
Calculate the magnitude of the unknown resistor RR.
R=4.0×60.040.0=6.0 ΩR = 4.0 \times \frac{60.0}{40.0} = 6.0\text{ }\Omega.
Multiplying and simplifying yields the exact resistance value.

Key Concept

Metre Bridge Principle (Wheatstone Bridge)
Question 60Question

A battery with an electromotive force (e.m.f.) of 9.0 V9.0\text{ V} and an internal resistance of 0.5 Ω0.5\text{ }\Omega is connected to an external circuit containing two resistors of 4.0 Ω4.0\text{ }\Omega and 1.5 Ω1.5\text{ }\Omega connected in series. What is the terminal potential difference across the battery?

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Answer: 8.25 V8.25\text{ V}

Answer

The terminal potential difference across the battery is 8.25 V8.25\text{ V}.
The correct answer is obtained by finding the total circuit resistance (6.0 Ω6.0\text{ }\Omega), determining the current (1.5 A1.5\text{ A}), and subtracting the internal voltage drop (0.75 V0.75\text{ V}) from the electromotive force (9.0 V9.0\text{ V}) to give 8.25 V8.25\text{ V}.

Step-by-Step Solution

1
Calculate the total resistance of the circuit.
Rtotal=R1+R2+r=4.0 Ω+1.5 Ω+0.5 Ω=6.0 ΩR_{\text{total}} = R_1 + R_2 + r = 4.0\text{ }\Omega + 1.5\text{ }\Omega + 0.5\text{ }\Omega = 6.0\text{ }\Omega
The external resistors and the battery's internal resistance are connected in series.
2
Calculate the total current flowing through the circuit using Ohm's Law.
I=ERtotal=9.0 V6.0 Ω=1.5 AI = \frac{E}{R_{\text{total}}} = \frac{9.0\text{ V}}{6.0\text{ }\Omega} = 1.5\text{ A}
The total current depends on the electromotive force and total circuit resistance.
3
Calculate the terminal potential difference across the battery.
V=EIr=9.0 V(1.5 A×0.5 Ω)=9.0 V0.75 V=8.25 VV = E - I r = 9.0\text{ V} - (1.5\text{ A} \times 0.5\text{ }\Omega) = 9.0\text{ V} - 0.75\text{ V} = 8.25\text{ V}
Terminal voltage is equal to the e.m.f. minus the potential drop across the internal resistance.

Key Concept

Terminal potential difference and internal resistance in DC electric circuits
Estimated Time:1m 30s
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