Electric Current and Resistance

24 questions

Question 1Question

A uniform metal wire of length 20m20\,\text{m} and total mass 0.034kg0.034\,\text{kg} is manufactured from a material of density 8.5×103kg/m38.5 \times 10^3\,\text{kg/m}^3 and electrical resistivity 1.7×108Ωm1.7 \times 10^{-8}\,\Omega\cdot\text{m}. What is the electrical resistance of the wire in ohms?

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Answer: 1.7

Answer

The electrical resistance of the wire is 1.7Ω1.7\,\Omega.
Combining the density relation V=mdV = \frac{m}{d} with the geometric expression V=ALV = A \cdot L gives A=mdLA = \frac{m}{d L}. Substituting this into Pouillet's law R=ρLAR = \frac{\rho L}{A} yields R=ρdL2mR = \frac{\rho d L^2}{m}. Evaluating with the given values: R=(1.7×108)(8.5×103)(20)20.034=1.7ΩR = \frac{(1.7 \times 10^{-8})(8.5 \times 10^3)(20)^2}{0.034} = 1.7\,\Omega.

Step-by-Step Solution

1
Calculate the volume of the wire using mass and density
V=4.0×106m3V = 4.0 \times 10^{-6}\,\text{m}^3
Volume is related to mass and density by V=mdV = \frac{m}{d}.
2
Calculate the cross-sectional area of the wire
A=2.0×107m2A = 2.0 \times 10^{-7}\,\text{m}^2
For a cylindrical wire of uniform cross-section, V=ALV = A \cdot L, so A=VLA = \frac{V}{L}.
3
Apply resistivity formula to find electrical resistance
R=1.7ΩR = 1.7\,\Omega
Resistance is given by R=ρLAR = \frac{\rho L}{A}.

Key Concept

Relationship between Resistance, Mass, Density, and Resistivity
Estimated Time:2m 0s
Question 2Question

Two cylindrical metallic conductors, XX and YY, are connected in series across a direct-current source. Wire XX has a diameter of 1.0mm1.0\,\text{mm} and a free-electron density of 6.0×1028m36.0 \times 10^{28}\,\text{m}^{-3}. Wire YY has a diameter of 3.0mm3.0\,\text{mm} and a free-electron density of 2.0×1028m32.0 \times 10^{28}\,\text{m}^{-3}. What is the ratio of the drift velocity of free electrons in wire XX to that in wire YY?

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Answer: 3.03.0

Answer

The ratio of the drift velocity in wire X to that in wire Y is 3.0.
Because the wires are connected in series, the same current passes through both (IX=IYI_X = I_Y). Using the formula for electric current in terms of drift velocity I=nAevdI = n A e v_d, where cross-sectional area A=πd2/4A = \pi d^2 / 4, we find vd1/(nd2)v_d \propto 1 / (n d^2). Taking the ratio yields vX/vY=(nYdY2)/(nXdX2)=(2.0×1028×3.02)/(6.0×1028×1.02)=18/6=3.0v_X / v_Y = (n_Y d_Y^2) / (n_X d_X^2) = (2.0 \times 10^{28} \times 3.0^2) / (6.0 \times 10^{28} \times 1.0^2) = 18 / 6 = 3.0.

Step-by-Step Solution

1
Relate electric current to drift velocity and conductor geometry.
I=nAevd=n(πd24)evdI = n A e v_d = n \left( \frac{\pi d^2}{4} \right) e v_d
Electric current II depends on free-electron density nn, cross-sectional area AA, elementary charge ee, and electron drift velocity vdv_d.
2
Apply the series connection constraint.
IX=IY    nXdX2vX=nYdY2vYI_X = I_Y \implies n_X d_X^2 v_X = n_Y d_Y^2 v_Y
In a series circuit, the steady current flowing through every conductor is identical.
3
Rearrange to solve for the drift velocity ratio vX/vYv_X / v_Y.
vXvY=nYdY2nXdX2\frac{v_X}{v_Y} = \frac{n_Y d_Y^2}{n_X d_X^2}
Isolating vX/vYv_X / v_Y demonstrates inverse proportionality to electron density and the square of conductor diameter.
4
Substitute the given values into the ratio expression.
\frac{v_X}{v_Y} = \frac{(2.0 \times 10^{28}\,\text{m}^{-3}) \times (3.0\,\text{mm})^2}{(6.0 \times 10^{28}\,\text{m}^{-3}) \times (1.0\,\text{mm})^2} = \frac{2.0 \times 9.0}{6.0 \times 1.0} = \frac{18.0}{6.0} = 3.0
Numerical calculation yields the simplified dimensionless ratio.

Key Concept

Drift Velocity and Current Density in Series Conductors
Question 3Question

A steady electric current of 2.5A2.5\,\text{A} flows through a conductor for 4.0minutes4.0\,\text{minutes}. What is the total electric charge that passes through any cross-section of the conductor during this period?

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Answer: 600C600\,\text{C}

Answer

600C600\,\text{C}
Electric current (II) is defined as the rate of charge flow (QQ) per unit time (tt), expressed as Q=I×tQ = I \times t. Converting 4.0minutes4.0\,\text{minutes} into seconds gives 4.0×60=240s4.0 \times 60 = 240\,\text{s}. Multiplying the current of 2.5A2.5\,\text{A} by 240s240\,\text{s} yields 600C600\,\text{C}.

Step-by-Step Solution

1
Convert the time duration from minutes to seconds
t=4.0minutes=4.0×60s=240secondst = 4.0\,\text{minutes} = 4.0 \times 60\,\text{s} = 240\,\text{seconds}
The standard SI unit for time in electromagnetism formulas is seconds.
2
Apply the formula relating electric charge, current, and time (Q=I×tQ = I \times t)
Q=2.5A×240s=600CQ = 2.5\,\text{A} \times 240\,\text{s} = 600\,\text{C}
Electric current is defined as the rate of flow of electric charge (I=QtI = \frac{Q}{t}).

Key Concept

Relationship between Electric Current, Charge, and Time
Question 4Question

A metallic wire has a resistance of 10.0Ω10.0\,\Omega at 0C0^\circ\text{C} and a temperature coefficient of resistance α=4.0×103K1\alpha = 4.0 \times 10^{-3}\,\text{K}^{-1}. The wire is uniformly stretched at constant temperature until its length is doubled while maintaining constant mass and volume. It is subsequently heated to 50C50^\circ\text{C}. What is the electric current, in Amperes, that flows through the wire when a potential difference of 120.0V120.0\,\text{V} is applied across its ends?

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Answer: 2.5

Answer

The electric current passing through the heated, stretched wire is 2.5 A.
When a wire of initial resistance 10.0 ohms is stretched to twice its original length, conservation of volume requires its cross-sectional area to halve, which quadruples its resistance to 40.0 ohms at 0 °C. Heating the wire by 50 K increases its resistance by a factor of (1 + 0.004 * 50) = 1.2, producing a final resistance of 48.0 ohms. Applying a 120.0 V potential difference across 48.0 ohms results in a current of 2.5 A.

Step-by-Step Solution

1
Determine resistance change due to wire stretching
R_0' = 40.0 ohms at 0 °C
Uniform stretching conserves total volume (V = A * L). Doubling length halves area, making resistance increase by a factor of 2^2 = 4.
2
Calculate resistance at 50 °C using temperature coefficient
R(50 °C) = 48.0 ohms
Resistance increases linearly with temperature: R(T) = R_0'(1 + alpha * Delta T).
3
Apply Ohm's law to find current
I = 2.5 A
Current is given by potential difference divided by total resistance at the operational temperature.

Key Concept

Resistance variation with geometric stretching and temperature coefficient of resistance
Question 5Question

A uniform metallic wire of resistance RR is stretched uniformly until its radius decreases by 20%20\%. The stretched wire is subsequently cut into two equal halves, which are then connected in parallel across a constant potential difference VV. What is the ratio of the total electrical power dissipated in this parallel combination to the power dissipated by the original unstretched wire under the same potential difference?

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Answer: 1.64

Answer

The ratio of the total power dissipated in the parallel combination to the original power is 1.64
When a wire of initial resistance RR is stretched so that its radius decreases by 20%20\%, its new radius is 0.8r0.8r. Because volume is conserved (A1L1=A2L2A_1 L_1 = A_2 L_2), reducing the cross-sectional area to 0.64A0.64A causes the length to increase to L/0.64L/0.64. Consequently, the resistance scales inversely with the fourth power of the radius: Rstretched=R/(0.8)4=R/0.4096=2.4414RR_{\text{stretched}} = R / (0.8)^4 = R / 0.4096 = 2.4414R. Cutting this wire into two equal pieces gives two resistors of 1.2207R1.2207R each. Connecting them in parallel yields an equivalent resistance Req=1.2207R/2=0.61035RR_{\text{eq}} = 1.2207R / 2 = 0.61035R. Power at constant voltage is P=V2/RP = V^2/R, so the new power is Pnew=V2/(0.61035R)=1.64(V2/R)=1.64PorigP_{\text{new}} = V^2 / (0.61035R) = 1.64 (V^2/R) = 1.64 P_{\text{orig}}.

Step-by-Step Solution

1
Determine the new resistance of the wire after stretching
Rstretched=R(0.8)4=R0.40962.4414RR_{\text{stretched}} = \frac{R}{(0.8)^4} = \frac{R}{0.4096} \approx 2.4414 R
Since mass and density remain constant, volume Vvol=ALV_{\text{vol}} = A \cdot L is conserved. Decreasing radius to r2=0.8r1r_2 = 0.8 r_1 reduces area to A2=0.64A1A_2 = 0.64 A_1 and increases length to L2=L1/0.64L_2 = L_1 / 0.64. Resistance R=ρL/A1/r4R = \rho L / A \propto 1/r^4.
2
Calculate the equivalent resistance of the two equal halves connected in parallel
Req=14Rstretched=2.4414R40.61035RR_{\text{eq}} = \frac{1}{4} R_{\text{stretched}} = \frac{2.4414 R}{4} \approx 0.61035 R
Cutting the stretched wire in half gives two pieces each of resistance Rhalf=Rstretched/2R_{\text{half}} = R_{\text{stretched}} / 2. Connecting two identical resistors in parallel yields an equivalent resistance Req=Rhalf/2=Rstretched/4R_{\text{eq}} = R_{\text{half}} / 2 = R_{\text{stretched}} / 4.
3
Calculate the ratio of power dissipated across a constant potential difference V
PnewPorig=V2/ReqV2/R=RReq=10.610351.64\frac{P_{\text{new}}}{P_{\text{orig}}} = \frac{V^2 / R_{\text{eq}}}{V^2 / R} = \frac{R}{R_{\text{eq}}} = \frac{1}{0.61035} \approx 1.64
Electrical power dissipated at constant voltage is given by P=V2/RP = V^2 / R, which means power is inversely proportional to equivalent resistance.

Key Concept

Dependence of electrical resistance on conductor geometry under volume conservation, and power dissipation in parallel circuits.
Question 6Question

A uniform conductor of length 50m50\,\text{m} and cross-sectional area 2.0×106m22.0 \times 10^{-6}\,\text{m}^2 is made of a material with a resistivity of 4.0×107Ωm4.0 \times 10^{-7}\,\Omega\cdot\text{m}. What is the electrical resistance of the conductor in ohms?

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Answer: 10

Answer

The resistance of the conductor is 10Ω10\,\Omega.
The resistance of a uniform conductor is given by R=ρLAR = \frac{\rho L}{A}. Substituting the values L=50mL = 50\,\text{m}, A=2.0×106m2A = 2.0 \times 10^{-6}\,\text{m}^2, and ρ=4.0×107Ωm\rho = 4.0 \times 10^{-7}\,\Omega\cdot\text{m} yields R=(4.0×107)(50)2.0×106=10ΩR = \frac{(4.0 \times 10^{-7})(50)}{2.0 \times 10^{-6}} = 10\,\Omega.

Step-by-Step Solution

1
Identify given physical quantities
L=50mL = 50\,\text{m}, A=2.0×106m2A = 2.0 \times 10^{-6}\,\text{m}^2, ρ=4.0×107Ωm\rho = 4.0 \times 10^{-7}\,\Omega\cdot\text{m}
Extracting given parameter values clearly sets up the mathematical relationship.
2
Apply the resistivity formula for resistance
R=ρLAR = \frac{\rho L}{A}
Resistance varies directly with length and resistivity, and inversely with cross-sectional area.
3
Perform the calculation
R=(4.0×107Ωm)(50m)2.0×106m2=10ΩR = \frac{(4.0 \times 10^{-7}\,\Omega\cdot\text{m})(50\,\text{m})}{2.0 \times 10^{-6}\,\text{m}^2} = 10\,\Omega
Multiplying the numerator gives 2.0×105Ωm22.0 \times 10^{-5}\,\Omega\cdot\text{m}^2; dividing by 2.0×106m22.0 \times 10^{-6}\,\text{m}^2 yields 10Ω10\,\Omega.

Key Concept

Direct computation of electrical resistance using resistivity, length, and cross-sectional area
Estimated Time:45s
Question 7Question

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 8Question

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 9Question

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 10Question

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 11Question

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 12Question

A uniform cylindrical metallic conductor has an initial resistance of 12.0Ω12.0\,\Omega. The conductor is stretched uniformly until its length increases by 50%50\%, while maintaining constant mass and density. If a constant potential difference of 27.0V27.0\,\text{V} is subsequently applied across the ends of the stretched conductor, what is the electric current passing through it?

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Answer: 1.0A1.0\,\text{A}

Answer

The electric current passing through the stretched conductor is 1.0A1.0\,\text{A}.
When a metallic conductor of fixed mass and volume is stretched, increasing its length by a factor of n=1.5n = 1.5 causes its cross-sectional area to decrease by a factor of 1.51.5. Because resistance is directly proportional to length and inversely proportional to cross-sectional area (R=ρL/AR = \rho L / A), the new resistance becomes n2n^2 times the initial resistance (1.52×12.0Ω=27.0Ω1.5^2 \times 12.0\,\Omega = 27.0\,\Omega). By Ohm's law, I=V/R=27.0V/27.0Ω=1.0AI = V / R = 27.0\,\text{V} / 27.0\,\Omega = 1.0\,\text{A}.

Step-by-Step Solution

1
Determine the new length and cross-sectional area of the stretched conductor
L2=1.5L1L_2 = 1.5 L_1 and A2=A11.5A_2 = \frac{A_1}{1.5}
Increasing the length by 50%50\% means L2=L1+0.5L1=1.5L1L_2 = L_1 + 0.5 L_1 = 1.5 L_1. Since the volume V=ALV = A \cdot L remains constant during stretching, A1L1=A2L2A_1 L_1 = A_2 L_2, which gives A2=A1/1.5A_2 = A_1 / 1.5.
2
Calculate the new resistance of the conductor
R2=27.0ΩR_2 = 27.0\,\Omega
Resistance is given by R=ρLAR = \rho \frac{L}{A}. Substituting the new length and area gives R2=ρ1.5L1A1/1.5=(1.5)2ρL1A1=2.25R1=2.25×12.0Ω=27.0ΩR_2 = \rho \frac{1.5 L_1}{A_1 / 1.5} = (1.5)^2 \rho \frac{L_1}{A_1} = 2.25 R_1 = 2.25 \times 12.0\,\Omega = 27.0\,\Omega.
3
Apply Ohm's law to find the current
I=1.0AI = 1.0\,\text{A}
Using I=VR2I = \frac{V}{R_2}, substitute V=27.0VV = 27.0\,\text{V} and R2=27.0ΩR_2 = 27.0\,\Omega to get I=27.0V27.0Ω=1.0AI = \frac{27.0\,\text{V}}{27.0\,\Omega} = 1.0\,\text{A}.

Key Concept

Resistance variation with length and cross-sectional area under constant volume constraint (RL2R \propto L^2 when stretched)
Estimated Time:2m 0s
Question 13Question

An electric iron draws a steady current of 2.5A2.5\,\text{A} when connected to a mains supply. What total electric charge passes through the heating element of the appliance in 2.0minutes2.0\,\text{minutes}?

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Answer: 300C300\,\text{C}

Answer

The total electric charge passing through the heating element is 300C300\,\text{C}.
Electric charge QQ is calculated using the formula Q=I×tQ = I \times t. Converting 2.0minutes2.0\,\text{minutes} into seconds gives 120s120\,\text{s}. Multiplying the current of 2.5A2.5\,\text{A} by 120s120\,\text{s} gives 300C300\,\text{C}.

Step-by-Step Solution

1
Convert the given time duration from minutes into seconds.
t=2.0minutes×60s/min=120st = 2.0\,\text{minutes} \times 60\,\text{s/min} = 120\,\text{s}.
Standard units require time to be measured in seconds when evaluating charge in coulombs.
2
Apply the electric charge formula Q=I×tQ = I \times t.
Q=2.5A×120s=300CQ = 2.5\,\text{A} \times 120\,\text{s} = 300\,\text{C}.
Electric current is defined as the total charge passing a given cross-section per unit time.

Key Concept

Electric Current and Charge Relationship
Question 14Question

A metallic conductor wire of cross-sectional area 2.5×106m22.5 \times 10^{-6}\,\text{m}^2 has a resistance of 10.0Ω10.0\,\Omega at 0C0\,^\circ\text{C}. The temperature coefficient of resistance of the material is 5.0×103C15.0 \times 10^{-3}\,^\circ\text{C}^{-1}. The conductor contains a free-electron density of 5.0×1028m35.0 \times 10^{28}\,\text{m}^{-3}. When the wire is heated to 100C100\,^\circ\text{C} and connected across a potential difference of 60V60\,\text{V}, what is the drift velocity of the conduction electrons in the wire in millimeters per second (mm/s\text{mm/s})? (Take elementary charge e=1.6×1019Ce = 1.6 \times 10^{-19}\,\text{C}.)

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Answer: 0.2

Answer

The drift velocity of the conduction electrons is 0.2mm/s0.2\,\text{mm/s}.
The resistance increases from 10.0Ω10.0\,\Omega to 15.0Ω15.0\,\Omega when heated from 0C0\,^\circ\text{C} to 100C100\,^\circ\text{C}. Applying 60V60\,\text{V} results in a current of 4.0A4.0\,\text{A}. Combining this with the cross-sectional area and electron density gives a drift velocity of 2.0×104m/s2.0 \times 10^{-4}\,\text{m/s}, which equals 0.2mm/s0.2\,\text{mm/s}.

Step-by-Step Solution

1
Calculate the resistance at the operating temperature (100C100\,^\circ\text{C})
R100=15.0ΩR_{100} = 15.0\,\Omega
Resistance varies with temperature according to RT=R0(1+αΔT)R_T = R_0(1 + \alpha \Delta T).
2
Find the current in the wire using Ohm's Law
I=4.0AI = 4.0\,\text{A}
Current is given by I=V/R100I = V / R_{100}.
3
Determine current density JJ
J=1.6×106A/m2J = 1.6 \times 10^6\,\text{A/m}^2
Current density is total current per unit cross-sectional area, J=I/AJ = I / A.
4
Calculate the electron drift velocity vdv_d
vd=2.0×104m/s=0.2mm/sv_d = 2.0 \times 10^{-4}\,\text{m/s} = 0.2\,\text{mm/s}
Drift velocity relates to current density by vd=J/(ne)v_d = J / (n e).

Key Concept

Temperature Dependence of Resistance and Microscopic Model of Electric Current
Estimated Time:2m 0s
Question 15Question

A resistor of resistance 15Ω15\,\Omega is connected across a direct-current source. If a steady current of 0.80A0.80\,\text{A} flows through the resistor, what is the potential difference across its terminals?

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Answer: 12V12\,\text{V}

Answer

The potential difference across the terminals of the resistor is 12V12\,\text{V}.
According to Ohm's law, the potential difference VV across a resistor is equal to the product of the electric current II passing through it and its resistance RR (V=I×RV = I \times R). Substituting I=0.80AI = 0.80\,\text{A} and R=15ΩR = 15\,\Omega yields V=12VV = 12\,\text{V}.

Step-by-Step Solution

1
Identify the given physical quantities
Resistance R=15ΩR = 15\,\Omega and electric current I=0.80AI = 0.80\,\text{A}.
These are the given parameters needed to find potential difference.
2
Apply Ohm's Law formula for potential difference
V=I×RV = I \times R
Ohm's law states that potential difference is directly proportional to current for a ohmic resistor of constant resistance.
3
Substitute the values and calculate
V=0.80A×15Ω=12VV = 0.80\,\text{A} \times 15\,\Omega = 12\,\text{V}
Multiplying current by resistance yields potential difference in volts.

Key Concept

Ohm's Law (V=IRV = IR)
Question 16Question

A resistance thermometer has a resistance of 4.0Ω4.0\,\Omega at 0C0\,^\circ\text{C} and 6.0Ω6.0\,\Omega at 100C100\,^\circ\text{C}. The thermometer is connected in series with a fixed 10.0Ω10.0\,\Omega resistor across a 24.0V24.0\,\text{V} DC power source having an internal resistance of 1.0Ω1.0\,\Omega. If a steady current of 1.2A1.2\,\text{A} flows through the circuit, what is the temperature of the thermometer's environment?

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Answer: 250C250\,^\circ\text{C}

Answer

The temperature of the thermometer environment is 250C250\,^\circ\text{C}.
By applying the complete circuit equation E=I(Rθ+Rfixed+r)E = I(R_\theta + R_{\text{fixed}} + r), the total circuit resistance is found to be 20.0Ω20.0\,\Omega. Subtracting the fixed resistance of 10.0Ω10.0\,\Omega and the cell internal resistance of 1.0Ω1.0\,\Omega yields the thermometer resistance Rθ=9.0ΩR_\theta = 9.0\,\Omega. Substituting this into the thermometric relation θ=RθR0R100R0×100C\theta = \frac{R_\theta - R_0}{R_{100} - R_0} \times 100\,^\circ\text{C} gives 9.04.06.04.0×100=250C\frac{9.0 - 4.0}{6.0 - 4.0} \times 100 = 250\,^\circ\text{C}.

Step-by-Step Solution

1
Calculate total circuit resistance using Ohm's Law and internal resistance equation
Rtotal=EI=24.0V1.2A=20.0ΩR_{\text{total}} = \frac{E}{I} = \frac{24.0\,\text{V}}{1.2\,\text{A}} = 20.0\,\Omega
The electromotive force (e.m.f) of the source equals total current multiplied by total resistance including internal resistance.
2
Determine the resistance of the thermometer at the unknown temperature (RθR_\theta)
Rθ=RtotalRfixedr=20.0Ω10.0Ω1.0Ω=9.0ΩR_\theta = R_{\text{total}} - R_{\text{fixed}} - r = 20.0\,\Omega - 10.0\,\Omega - 1.0\,\Omega = 9.0\,\Omega
The circuit components are in series, so total resistance is the sum of external resistances and internal resistance.
3
Apply the linear resistance thermometer temperature scale formula
\(\theta = \frac{R_\theta - R_0}{R_{100} - R_0} \times 100\,^\circ\text{C} = \frac{9.0 - 4.0}{6.0 - 4.0} \times 100 = \frac{5.0}{2.0} \times 100 = 250\,^\circ\text{C}\)
Resistance varies linearly with temperature between the ice point (0C0\,^\circ\text{C}) and steam point (100C100\,^\circ\text{C}).

Key Concept

Integration of Ohm's Law, internal resistance of a cell, and resistance thermometry
Estimated Time:2m 0s
Question 17Question

A conductor wire with a cross-sectional area of 2.0×106m22.0 \times 10^{-6}\,\text{m}^2 carries a steady current of 1.6A1.6\,\text{A}. If the conduction electron density of the material is 5.0×1028m35.0 \times 10^{28}\,\text{m}^{-3} and the elementary charge is 1.6×1019C1.6 \times 10^{-19}\,\text{C}, what is the average drift velocity of the electrons in the wire?

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Answer: 1.0×104m/s1.0 \times 10^{-4}\,\text{m/s}

Answer

The average drift velocity of the electrons is 1.0×104m/s1.0 \times 10^{-4}\,\text{m/s}.
The correct answer is derived from the fundamental relationship I=nAevdI = n A e v_d. Solving for drift velocity gives vd=InAe=1.65.0×1028×2.0×106×1.6×1019=1.0×104m/sv_d = \frac{I}{n A e} = \frac{1.6}{5.0 \times 10^{28} \times 2.0 \times 10^{-6} \times 1.6 \times 10^{-19}} = 1.0 \times 10^{-4}\,\text{m/s}.

Step-by-Step Solution

1
Identify the drift velocity formula relating current to charge carrier parameters
The electric current is given by I=nAevdI = n A e v_d, where II is current, nn is electron density, AA is cross-sectional area, ee is elementary charge, and vdv_d is drift velocity.
This formula connects macroscopic electric current to microscopic charge dynamics.
2
Rearrange the equation to solve for drift velocity vdv_d
vd=InAev_d = \frac{I}{n A e}
Isolating the unknown variable vdv_d before substituting known values.
3
Substitute the given values into the expression
vd=1.6(5.0×1028)×(2.0×106)×(1.6×1019)v_d = \frac{1.6}{(5.0 \times 10^{28}) \times (2.0 \times 10^{-6}) \times (1.6 \times 10^{-19})}
Inserting I=1.6AI = 1.6\,\text{A}, n=5.0×1028m3n = 5.0 \times 10^{28}\,\text{m}^{-3}, A=2.0×106m2A = 2.0 \times 10^{-6}\,\text{m}^2, and e=1.6×1019Ce = 1.6 \times 10^{-19}\,\text{C}.
4
Evaluate the denominator and compute the final value of vdv_d
Denominator =(5.0×2.0×1.6)×1028619=16.0×103=1.6×104= (5.0 \times 2.0 \times 1.6) \times 10^{28 - 6 - 19} = 16.0 \times 10^3 = 1.6 \times 10^4. Thus, vd=1.61.6×104=1.0×104m/sv_d = \frac{1.6}{1.6 \times 10^4} = 1.0 \times 10^{-4}\,\text{m/s}.
Simplifying powers of ten gives the final numerical answer.

Key Concept

Relationship between Electric Current and Drift Velocity
Estimated Time:1m 30s
Question 18Question

Two cylindrical wires, X and Y, are made of the same uniform conducting material. Wire X has length LL, diameter dd, and an electrical resistance of 12Ω12\,\Omega. Wire Y has length 2L2L and diameter 2d2d. What is the resistance of wire Y?

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Answer: 6Ω6\,\Omega

Answer

The resistance of wire Y is 6Ω6\,\Omega.
The resistance of a uniform conductor is given by R=4ρLπd2R = \frac{4\rho L}{\pi d^2}. For wire X, RX=12ΩR_X = 12\,\Omega. For wire Y with length 2L2L and diameter 2d2d, the new resistance becomes RY=4ρ(2L)π(2d)2=8ρL4πd2=12(4ρLπd2)=12RX=6ΩR_Y = \frac{4\rho(2L)}{\pi (2d)^2} = \frac{8\rho L}{4\pi d^2} = \frac{1}{2}\left(\frac{4\rho L}{\pi d^2}\right) = \frac{1}{2} R_X = 6\,\Omega.

Step-by-Step Solution

1
Express the resistance of a cylindrical conductor in terms of length LL and diameter dd.
R=ρLA=ρLπ(d/2)2=4ρLπd2R = \rho \frac{L}{A} = \rho \frac{L}{\pi (d/2)^2} = \frac{4\rho L}{\pi d^2}
The cross-sectional area AA of a circular wire with diameter dd is given by A=πd24A = \frac{\pi d^2}{4}.
2
Write the resistance formula for wire X using its given value.
RX=4ρLπd2=12ΩR_X = \frac{4\rho L}{\pi d^2} = 12\,\Omega
Wire X has length LL and diameter dd.
3
Substitute the parameters of wire Y (LY=2LL_Y = 2L and dY=2dd_Y = 2d) into the resistance formula.
RY=4ρ(2L)π(2d)2=8ρL4πd2=2ρLπd2R_Y = \frac{4\rho (2L)}{\pi (2d)^2} = \frac{8\rho L}{4\pi d^2} = \frac{2\rho L}{\pi d^2}
Doubling diameter increases the cross-sectional area by a factor of 22=42^2 = 4.
4
Relate the resistance of wire Y to the resistance of wire X and calculate the final numerical value.
RY=12(4ρLπd2)=12RX=12Ω2=6ΩR_Y = \frac{1}{2} \left(\frac{4\rho L}{\pi d^2}\right) = \frac{1}{2} R_X = \frac{12\,\Omega}{2} = 6\,\Omega
Since RY=12RXR_Y = \frac{1}{2} R_X, halving 12Ω12\,\Omega yields 6Ω6\,\Omega.

Key Concept

Dependence of Electrical Resistance on Conductor Dimensions
Estimated Time:1m 30s
Question 19Question

A metallic wire has a resistance of 12.0Ω12.0\,\Omega at 0C0\,^\circ\text{C} and a temperature coefficient of resistance of 4.0×103C14.0 \times 10^{-3}\,^\circ\text{C}^{-1}. The wire is uniformly stretched until its length increases by 25%25\%. Assuming the density and total volume of the wire remain constant during stretching, what is the resistance of the stretched wire at 50C50\,^\circ\text{C}?

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Answer: 22.5

Answer

The resistance of the stretched wire at 50C50\,^\circ\text{C} is 22.5Ω22.5\,\Omega.
Stretching a wire by 25%25\% increases its length by a factor of 1.251.25 and reduces its cross-sectional area by a factor of 1.251.25 (since volume is conserved). The resistance at 0C0\,^\circ\text{C} scales as (1.25)2=1.5625(1.25)^2 = 1.5625, giving 18.75Ω18.75\,\Omega. Accounting for the temperature increase to 50C50\,^\circ\text{C} via R(T)=R0(1+αT)R(T) = R'_0(1 + \alpha T) yields 18.75×(1+4.0×103×50)=18.75×1.20=22.5Ω18.75 \times (1 + 4.0 \times 10^{-3} \times 50) = 18.75 \times 1.20 = 22.5\,\Omega.

Step-by-Step Solution

1
Calculate the resistance of the wire at 0C0\,^\circ\text{C} after uniform stretching.
R0=18.75ΩR'_0 = 18.75\,\Omega
Uniform stretching by 25%25\% increases length to L=1.25L0L' = 1.25 L_0. Volume conservation (V=ALV = A L) requires area to decrease to A=A0/1.25A' = A_0 / 1.25. Since R=ρL/AR = \rho L / A, R0=R0(L/L0)2=12.0×(1.25)2=18.75ΩR'_0 = R_0 (L'/L_0)^2 = 12.0 \times (1.25)^2 = 18.75\,\Omega.
2
Apply the temperature coefficient formula to calculate resistance at 50C50\,^\circ\text{C}.
R(50)=22.5ΩR(50) = 22.5\,\Omega
Using R(T)=R0(1+αT)R(T) = R'_0 (1 + \alpha T), substitute R0=18.75ΩR'_0 = 18.75\,\Omega, α=4.0×103C1\alpha = 4.0 \times 10^{-3}\,^\circ\text{C}^{-1}, and T=50CT = 50\,^\circ\text{C} to find R(50)=18.75×(1+0.20)=22.5ΩR(50) = 18.75 \times (1 + 0.20) = 22.5\,\Omega.

Key Concept

Combined effects of dimensional deformation and temperature on electrical resistance
Question 20Question

A uniform metallic conductor of length 200m200\,\text{m} and cross-sectional area 2.0×106m22.0 \times 10^{-6}\,\text{m}^2 has a resistivity of 1.6×108Ωm1.6 \times 10^{-8}\,\Omega\cdot\text{m} at an initial temperature of 20C20\,^\circ\text{C}. The temperature coefficient of resistivity for the material is 5.0×103C15.0 \times 10^{-3}\,^\circ\text{C}^{-1}. If the operating temperature of the conductor increases to 120C120\,^\circ\text{C} while it is connected across a constant potential difference of 12V12\,\text{V}, what is the magnitude of the electric current flowing through the conductor in amperes?

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Answer: 5

Answer

The electric current flowing through the conductor is 5.0A5.0\,\text{A}.
The temperature change of 100C100\,^\circ\text{C} increases the resistivity of the material from 1.6×108Ωm1.6 \times 10^{-8}\,\Omega\cdot\text{m} to 2.4×108Ωm2.4 \times 10^{-8}\,\Omega\cdot\text{m} via ρ=ρ0(1+αΔT)\rho = \rho_0(1 + \alpha \Delta T). Substituting this updated resistivity into R=ρLAR = \frac{\rho L}{A} gives a resistance of 2.4Ω2.4\,\Omega. Applying Ohm's Law I=VRI = \frac{V}{R} with a potential difference of 12V12\,\text{V} yields 5.0A5.0\,\text{A}.

Step-by-Step Solution

1
Calculate the temperature difference
ΔT=100C\Delta T = 100\,^\circ\text{C}
The temperature change relative to the reference temperature dictates the change in resistivity.
2
Calculate the resistivity at the final temperature
ρ=2.4×108Ωm\rho = 2.4 \times 10^{-8}\,\Omega\cdot\text{m}
Resistivity depends on temperature according to ρ=ρ0(1+αΔT)\rho = \rho_0(1 + \alpha \Delta T).
3
Calculate the total electrical resistance of the conductor
R = 2.4\,\Omega
Resistance is related to physical geometry and resistivity by R=ρLAR = \frac{\rho L}{A}.
4
Apply Ohm's law to solve for the current
I = 5.0\,\text{A}
Electric current is determined by potential difference divided by resistance (I=V/RI = V / R).

Key Concept

Temperature dependence of resistivity and Ohm's Law
Estimated Time:2m 0s
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