Electricity and Magnetism

198 questions

Question 61Question

A DC supply with an electromotive force (e.m.f.) of 24.0 V24.0\text{ V} and an internal resistance of 2.0 Ω2.0\text{ }\Omega is connected across three identical 12.0 Ω12.0\text{ }\Omega resistors connected in parallel. What is the terminal potential difference across the battery in volts?

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Answer: 16

Answer

The terminal potential difference across the battery is 16.0 V16.0\text{ V}.
The three identical 12.0 Ω12.0\text{ }\Omega resistors in parallel combine to yield an equivalent external resistance of 4.0 Ω4.0\text{ }\Omega. Adding the battery's internal resistance of 2.0 Ω2.0\text{ }\Omega gives a total circuit resistance of 6.0 Ω6.0\text{ }\Omega. The total current drawn from the battery is I=24.0 V6.0 Ω=4.0 AI = \frac{24.0\text{ V}}{6.0\text{ }\Omega} = 4.0\text{ A}. The terminal potential difference is the voltage drop across the external circuit, V=4.0 A×4.0 Ω=16.0 VV = 4.0\text{ A} \times 4.0\text{ }\Omega = 16.0\text{ V}.

Step-by-Step Solution

1
Find the equivalent external resistance of the three parallel resistors.
Rp=4.0 ΩR_p = 4.0\text{ }\Omega
Three identical resistors R=12.0 ΩR = 12.0\text{ }\Omega connected in parallel have an equivalent resistance of Rp=12.03=4.0 ΩR_p = \frac{12.0}{3} = 4.0\text{ }\Omega.
2
Find the total circuit resistance by adding internal resistance to the parallel combination.
Rtotal=6.0 ΩR_{total} = 6.0\text{ }\Omega
Internal resistance r=2.0 Ωr = 2.0\text{ }\Omega acts in series with the external parallel combination: Rtotal=Rp+r=4.0+2.0=6.0 ΩR_{total} = R_p + r = 4.0 + 2.0 = 6.0\text{ }\Omega.
3
Calculate the total current supplied by the cell.
I=4.0 AI = 4.0\text{ A}
Using the circuit formula I=ERtotalI = \frac{E}{R_{total}}, we divide the e.m.f. of 24.0 V24.0\text{ V} by the total resistance of 6.0 Ω6.0\text{ }\Omega.
4
Compute the terminal potential difference across the cell.
V=16.0 VV = 16.0\text{ V}
The potential drop across the external parallel network is V=IRp=4.0 A×4.0 Ω=16.0 VV = I R_p = 4.0\text{ A} \times 4.0\text{ }\Omega = 16.0\text{ V}, which equals EIr=24.0 V(4.0 A×2.0 Ω)=16.0 VE - Ir = 24.0\text{ V} - (4.0\text{ A} \times 2.0\text{ }\Omega) = 16.0\text{ V}.

Key Concept

Terminal Potential Difference and Internal Resistance
Estimated Time:1m 30s
Question 62Question

An electric circuit consists of a voltage source with an electromotive force (e.m.f.) of 6.0 V6.0\text{ V} and an internal resistance of 1.0 Ω1.0\text{ }\Omega connected across two identical 6.0 Ω6.0\text{ }\Omega resistors arranged in parallel. If an ammeter of negligible resistance is connected in series with the voltage source, what current will be displayed on the ammeter?

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Answer: 1.5 A1.5\text{ A}

Answer

The ammeter will record a total main circuit current of 1.5 A1.5\text{ A}.
The correct response demonstrates proper circuit reduction. First, combining the two 6.0 Ω6.0\text{ }\Omega parallel resistors gives an equivalent resistance of 3.0 Ω3.0\text{ }\Omega. Second, adding the 1.0 Ω1.0\text{ }\Omega internal resistance yields a total resistance of 4.0 Ω4.0\text{ }\Omega. Applying Ohm's law (I=ER+rI = \frac{E}{R+r}) gives I=6.0 V4.0 Ω=1.5 AI = \frac{6.0\text{ V}}{4.0\text{ }\Omega} = 1.5\text{ A}, which is the total current measured by an ammeter placed in the main circuit.

Step-by-Step Solution

1
Calculate the equivalent external resistance (RpR_p) of the two parallel resistors.
Rp=6.0×6.06.0+6.0=36.012.0=3.0 ΩR_p = \frac{6.0 \times 6.0}{6.0 + 6.0} = \frac{36.0}{12.0} = 3.0\text{ }\Omega
Resistors in parallel combine according to 1Rp=1R1+1R2\frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2}.
2
Determine the total resistance (RtotalR_{\text{total}}) of the complete circuit, including internal resistance.
Rtotal=Rp+r=3.0 Ω+1.0 Ω=4.0 ΩR_{\text{total}} = R_p + r = 3.0\text{ }\Omega + 1.0\text{ }\Omega = 4.0\text{ }\Omega
Internal resistance acts in series with the equivalent external load resistance.
3
Apply Ohm's law for a complete circuit to find the total current (II).
I=ERtotal=6.0 V4.0 Ω=1.5 AI = \frac{E}{R_{\text{total}}} = \frac{6.0\text{ V}}{4.0\text{ }\Omega} = 1.5\text{ A}
The total current supplied by the source equals the electromotive force divided by the total circuit resistance.

Key Concept

Terminal Circuit Current with Internal Resistance and Parallel Resistor Combinations
Question 63Question

An electric iron rated at 1200W1200\,\text{W} is operated for 5hours5\,\text{hours} each day for a period of 30days30\,\text{days}. If electrical energy costs 20.00\text{₦}20.00 per kilowatt-hour (kWh\text{kWh}), what is the total cost of electricity consumed by the iron over this period in Naira (\text{₦})?

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Answer: 3600

Answer

The total cost of electricity consumed by the iron over the 30-day period is 3600 Naira.
To find the cost of electrical energy in commercial units, express power in kilowatts (1.2kW1.2\,\text{kW}) and time in total hours (150h150\,\text{h}). The energy consumed is 1.2×150=180kWh1.2 \times 150 = 180\,\text{kWh}. At a tariff of 20.00\text{₦}20.00 per kWh\text{kWh}, the total cost is 180×20=3600Naira180 \times 20 = 3600\,\text{Naira}.

Step-by-Step Solution

1
Convert the power rating of the appliance from watts to kilowatts
P=1200W1000=1.2kWP = \frac{1200\,\text{W}}{1000} = 1.2\,\text{kW}
Commercial energy consumption is calculated in kilowatt-hours (kWh), requiring power in kilowatts.
2
Calculate the total operating time in hours
t=5hours/day×30days=150hourst = 5\,\text{hours/day} \times 30\,\text{days} = 150\,\text{hours}
The usage duration across the month must be expressed in total hours.
3
Determine electrical energy consumed in kWh
E=P×t=1.2kW×150h=180kWhE = P \times t = 1.2\,\text{kW} \times 150\,\text{h} = 180\,\text{kWh}
Energy is the product of power in kilowatts and time in hours.
4
Calculate total cost of energy consumed
Total Cost=180kWh×20.00/kWh=3600\text{Total Cost} = 180\,\text{kWh} \times \text{₦}20.00/\text{kWh} = \text{₦}3600
Total cost is found by multiplying energy in kWh by the unit tariff rate.

Key Concept

Commercial electrical energy unit (kWh) and billing calculation
Question 64Question

Two electric lamps rated at 60W,220V60\,\text{W}, 220\,\text{V} and 100W,220V100\,\text{W}, 220\,\text{V} respectively are connected in series across a 220V220\,\text{V} supply line. What is the total electric power dissipated by the combination?

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Answer: 37.5W37.5\,\text{W}

Answer

The total electric power dissipated by the two lamps in series is 37.5W37.5\,\text{W}.
For two appliances designed for the same rated voltage VV connected in series across that voltage VV, the equivalent power is given by the formula Ptotal=P1P2P1+P2P_{\text{total}} = \frac{P_1 P_2}{P_1 + P_2}. Substituting P1=60WP_1 = 60\,\text{W} and P2=100WP_2 = 100\,\text{W} gives Ptotal=60×10060+100=37.5WP_{\text{total}} = \frac{60 \times 100}{60 + 100} = 37.5\,\text{W}.

Step-by-Step Solution

1
Calculate the resistance of each lamp from its rating.
R1=V2P1=220260=806.67ΩR_1 = \frac{V^2}{P_1} = \frac{220^2}{60} = 806.67\,\Omega and R2=V2P2=2202100=484.00ΩR_2 = \frac{V^2}{P_2} = \frac{220^2}{100} = 484.00\,\Omega
Electrical devices are rated at a specific voltage, allowing their resistance to be determined via R=V2PR = \frac{V^2}{P}.
2
Find the total resistance of the series circuit.
Rtotal=R1+R2=806.67+484.00=1290.67ΩR_{\text{total}} = R_1 + R_2 = 806.67 + 484.00 = 1290.67\,\Omega
Resistors in series add directly.
3
Calculate total power drawn from the 220V220\,\text{V} supply.
Ptotal=V2Rtotal=22021290.67=37.5WP_{\text{total}} = \frac{V^2}{R_{\text{total}}} = \frac{220^2}{1290.67} = 37.5\,\text{W}
Total power is total voltage squared divided by equivalent resistance.

Key Concept

Power combination in series circuits
Estimated Time:1m 30s
Question 65Question

Match each electrical operational scenario on the left with its corresponding effect on electrical energy or power on the right.

Click a left item, then click its matching right item

Items

Doubling the electric current passing through a resistor of constant resistance for a fixed duration
Halving the operating potential difference applied across a resistor of constant resistance
Connecting two identical resistors in parallel across a constant voltage source
Operating a 500W500\,\text{W} appliance continuously for a duration of 2hours2\,\text{hours}

Matches

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Answer

Doubling current quadruples heat energy (HI2H \propto I^2); halving voltage reduces power to one-quarter (PV2P \propto V^2); connecting two identical resistors in parallel doubles total power (P1/ReqP \propto 1/R_{\text{eq}}); and operating a 500 W appliance for 2 hours consumes 1.0 kWh.
Each left-side scenario correctly aligns with fundamental laws of electrical energy and power: doubling current quadruples heat energy via HI2H \propto I^2; halving voltage reduces power to one-quarter via PV2P \propto V^2; parallel resistor connection halves total resistance and doubles power; and operating a 0.5 kW appliance for 2 hours consumes 1.0 kWh.

Step-by-Step Solution

1
Apply Joule's Law of Heating (H=I2RtH = I^2 R t) to determine the effect of changing current.
Doubling current from II to 2I2I results in H=(2I)2Rt=4I2Rt=4HH' = (2I)^2 R t = 4 I^2 R t = 4H, so heat quadruples.
Heat generation depends on the square of current when resistance and time are constant.
2
Apply the voltage-power relationship (P=V2RP = \frac{V^2}{R}) for changing voltage.
Halving potential difference to V/2V/2 yields P=(V/2)2R=V24R=P4P' = \frac{(V/2)^2}{R} = \frac{V^2}{4R} = \frac{P}{4}, so power drops to one-quarter.
Power is directly proportional to the square of potential difference across a constant resistance.
3
Calculate parallel resistance and total circuit power.
Equivalent resistance of two parallel resistors is R/2R/2. Total power is Ptotal=V2R/2=2V2RP_{\text{total}} = \frac{V^2}{R/2} = 2 \frac{V^2}{R}, which is double the single resistor power.
Parallel combination reduces net resistance by half, thereby doubling total current and power drawn from a constant voltage source.
4
Calculate energy consumption in commercial units (kWh).
E=0.5kW×2h=1.0kWhE = 0.5\,\text{kW} \times 2\,\text{h} = 1.0\,\text{kWh}.
Commercial energy is computed by expressing power in kW and time in hours.

Key Concept

Mathematical relationships governing electrical power (P=I2R=V2RP = I^2 R = \frac{V^2}{R}), Joule heating (H=I2RtH = I^2 R t), and commercial energy units (kWh).
Question 66Question

A dip needle placed in the magnetic meridian at a location on the Earth's surface makes an angle of 3030^\circ with the horizontal. If the total intensity of the Earth's magnetic field at this location is 6.0×105 T6.0 \times 10^{-5}\text{ T}, what is the vertical component of the Earth's magnetic field?

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Answer: 3.0×105 T3.0 \times 10^{-5}\text{ T}

Answer

The vertical component of the Earth's magnetic field is 3.0×105 T3.0 \times 10^{-5}\text{ T}.
The vertical component of the Earth's magnetic field is given by Bv=BsinθB_v = B \sin \theta. Substituting B=6.0×105 TB = 6.0 \times 10^{-5}\text{ T} and θ=30\theta = 30^\circ yields Bv=6.0×105×0.5=3.0×105 TB_v = 6.0 \times 10^{-5} \times 0.5 = 3.0 \times 10^{-5}\text{ T}.

Step-by-Step Solution

1
Identify the given physical quantities from the problem statement.
Total intensity B=6.0×105 TB = 6.0 \times 10^{-5}\text{ T} and inclination angle θ=30\theta = 30^\circ.
These parameters are required to compute the resolved component.
2
Recall the formula for resolving the vertical component of Earth's magnetic field.
Bv=BsinθB_v = B \sin \theta
The vertical component corresponds to the vertical side of the right triangle formed by total field BB and angle of dip θ\theta.
3
Substitute the given values into the formula and calculate.
Bv=(6.0×105 T)×sin(30)=(6.0×105)×0.5=3.0×105 TB_v = (6.0 \times 10^{-5}\text{ T}) \times \sin(30^\circ) = (6.0 \times 10^{-5}) \times 0.5 = 3.0 \times 10^{-5}\text{ T}.
Since sin(30)=0.5\sin(30^\circ) = 0.5, multiplying 6.0×1056.0 \times 10^{-5} by 0.50.5 yields 3.0×105 T3.0 \times 10^{-5}\text{ T}.

Key Concept

Resolution of Earth's total magnetic field into horizontal and vertical components
Question 67Question

An electric heating element rated at 1000W1000\,\text{W} and 220V220\,\text{V} is connected to a 110V110\,\text{V} power line. Assuming the electrical resistance of the heating element remains constant, what is the power dissipated by the heater when operating at this reduced voltage?

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Answer: 250W250\,\text{W}

Answer

250W250\,\text{W}
The electrical power rating of an appliance defines its fixed resistance via R=V2PR = \frac{V^2}{P}. With R=48.4ΩR = 48.4\,\Omega, connecting the appliance to a 110V110\,\text{V} supply yields P=110248.4=250WP = \frac{110^2}{48.4} = 250\,\text{W}. Alternatively, because PV2P \propto V^2 for a constant resistance, halving the voltage reduces the power by a factor of (1/2)2=1/4(1/2)^2 = 1/4, giving 1000W×14=250W1000\,\text{W} \times \frac{1}{4} = 250\,\text{W}.

Step-by-Step Solution

1
Calculate the resistance RR of the heater from its rated values.
R=Vrated2Prated=22021000=484001000=48.4ΩR = \frac{V_{\text{rated}}^2}{P_{\text{rated}}} = \frac{220^2}{1000} = \frac{48400}{1000} = 48.4\,\Omega
The resistance of a heating element is determined by its physical design and rated specifications.
2
Calculate the power PnewP_{\text{new}} dissipated when connected to the 110V110\,\text{V} supply.
Pnew=Vnew2R=110248.4=1210048.4=250WP_{\text{new}} = \frac{V_{\text{new}}^2}{R} = \frac{110^2}{48.4} = \frac{12100}{48.4} = 250\,\text{W}
Electric power dissipated across a constant resistance varies with the square of the applied voltage.

Key Concept

Relationship between voltage, resistance, and electrical power dissipation
Estimated Time:1m 30s
Question 68Question

At a magnetic observation station, the horizontal component of the Earth's magnetic field is 40 μT40\text{ }\mu\text{T} and the vertical component is 30 μT30\text{ }\mu\text{T}. What is the total magnetic field intensity of the Earth at this station in μT\mu\text{T}?

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Answer: 50

Answer

The total magnetic field intensity of the Earth at this station is 50 μT50\text{ }\mu\text{T}.
The horizontal component (BhB_h) and vertical component (BvB_v) of the Earth's magnetic field act at right angles to each other. Therefore, the resultant total magnetic field intensity (BB) is calculated using vector addition: B=Bh2+Bv2=402+302=50 μTB = \sqrt{B_h^2 + B_v^2} = \sqrt{40^2 + 30^2} = 50\text{ }\mu\text{T}.

Step-by-Step Solution

1
Identify the vector relationship between the horizontal and vertical components of the Earth's magnetic field.
B=Bh2+Bv2B = \sqrt{B_h^2 + B_v^2}, where Bh=40 μTB_h = 40\text{ }\mu\text{T} and Bv=30 μTB_v = 30\text{ }\mu\text{T}.
The horizontal and vertical components of the Earth's magnetic field are mutually perpendicular vector components.
2
Substitute the values into the formula and solve for total magnetic field intensity BB.
B=(40)2+(30)2=1600+900=2500=50 μTB = \sqrt{(40)^2 + (30)^2} = \sqrt{1600 + 900} = \sqrt{2500} = 50\text{ }\mu\text{T}.
Applying the Pythagorean theorem yields the magnitude of the resultant magnetic field vector.

Key Concept

Resolution of Earth's magnetic field into horizontal (BhB_h) and vertical (BvB_v) components.
Estimated Time:1m 0s
Question 69Question

At the Earth's magnetic poles, the horizontal component of the Earth's magnetic field reaches its maximum value while the vertical component is equal to zero.

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Answer: False

Answer

The statement is false. At the magnetic poles, the angle of dip is 9090^\circ, which means the horizontal component of the Earth's magnetic field is zero and the vertical component is at its maximum.
The statement is false because at the Earth's magnetic poles, the angle of inclination (dip) is 9090^\circ. Substituting this angle into the component resolution formulas yields Bh=Bcos90=0B_h = B \cos 90^\circ = 0 and Bv=Bsin90=BB_v = B \sin 90^\circ = B. Therefore, the horizontal component is zero and the vertical component is maximum at the poles.

Step-by-Step Solution

1
Determine the angle of dip (θ\theta) at the Earth's magnetic poles.
The angle of dip at the poles is θ=90\theta = 90^\circ.
The Earth's magnetic flux lines enter or leave the surface vertically at the magnetic poles.
2
Calculate the horizontal component (BhB_h) using the magnetic field resolution formula.
Bh=Bcos(90)=0B_h = B \cos(90^\circ) = 0.
Since cos(90)=0\cos(90^\circ) = 0, there is no horizontal magnetic field component at the poles.
3
Calculate the vertical component (BvB_v) using the magnetic field resolution formula.
Bv=Bsin(90)=BB_v = B \sin(90^\circ) = B.
Since sin(90)=1\sin(90^\circ) = 1, the vertical component accounts for the entire total magnetic field intensity.
4
Compare the calculated component values against the given statement.
The statement claims BhB_h is maximum and Bv=0B_v = 0, which contradicts the physical reality where Bh=0B_h = 0 and BvB_v is maximum.
Therefore, the statement is evaluated as false.

Key Concept

Earth's Magnetic Field Components at Magnetic Poles
Question 70Question

According to Lenz's law, what occurs at the near face of a stationary solenoid when the north pole of a bar magnet is moved rapidly towards it?

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Answer: A magnetic north pole is induced at the near face to oppose the approaching magnet.

Answer

A magnetic north pole is induced at the near face to oppose the approaching magnet.
Lenz's law states that the direction of an induced current is always such that its magnetic effect opposes the motion or change causing it. When a north pole approaches the solenoid face, the induced current flows counter-clockwise (viewed from the magnet) to form an induced magnetic north pole at that face, thereby exerting a repulsive force that opposes the motion.

Step-by-Step Solution

1
Identify the cause of change in magnetic flux.
The approaching north pole increases magnetic flux linking the solenoid.
Electromagnetic induction occurs whenever magnetic flux linked with a conductor changes.
2
Apply Lenz's law to determine the polarity of the induced field.
The induced current must produce a magnetic field that opposes the increase in flux caused by the approaching north pole.
Lenz's law states that the induced effect always opposes the cause producing it.
3
Deduce the required magnetic pole at the near face.
A north pole must be set up at the near face because like magnetic poles repel each other, opposing the inward motion.
Repulsion between like poles (North against North) exerts a retarding force on the approaching magnet.

Key Concept

Lenz's Law of Electromagnetic Induction
Question 71Question

Two point charges, q1=+1.6×108 Cq_1 = +1.6 \times 10^{-8}\text{ C} and q2=+6.4×108 Cq_2 = +6.4 \times 10^{-8}\text{ C}, are fixed in a vacuum at a distance of 0.60 m0.60\text{ m} apart. At what distance from q1q_1 along the line joining the two charges is the net electric field intensity equal to zero?

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Answer: 0.20 m0.20\text{ m}

Answer

The distance from q1q_1 where the net electric field intensity is zero is 0.20 m0.20\text{ m}.
The net electric field is zero where the magnitudes of the electric fields produced by both charges are equal (E1=E2E_1 = E_2). Setting up kq1x2=kq2(0.60x)2\frac{k q_1}{x^2} = \frac{k q_2}{(0.60 - x)^2} with q2=4q1q_2 = 4 q_1 yields 1x2=4(0.60x)2\frac{1}{x^2} = \frac{4}{(0.60 - x)^2}. Taking the square root gives 1x=20.60x\frac{1}{x} = \frac{2}{0.60 - x}, which yields x=0.20 mx = 0.20\text{ m} from q1q_1.

Step-by-Step Solution

1
Set up the condition for zero net electric field intensity.
The electric field magnitudes produced by q1q_1 and q2q_2 at distance xx from q1q_1 must be equal in magnitude and opposite in direction: E1=E2E_1 = E_2.
Since both charges are positive, the point of zero net electric field must lie on the line segment connecting them.
2
Substitute the electric field formula into the equilibrium equation.
kq1x2=kq2(dx)2\frac{k q_1}{x^2} = \frac{k q_2}{(d - x)^2}, where d=0.60 md = 0.60\text{ m}.
Electric field intensity due to a point charge is given by E=kqr2E = \frac{k q}{r^2}.
3
Simplify the equation by canceling common terms and substituting known charge values.
1.6×108x2=6.4×108(0.60x)2    1x2=4(0.60x)2\frac{1.6 \times 10^{-8}}{x^2} = \frac{6.4 \times 10^{-8}}{(0.60 - x)^2} \implies \frac{1}{x^2} = \frac{4}{(0.60 - x)^2}.
Dividing both sides by k×1.6×108k \times 1.6 \times 10^{-8} reduces the numerical coefficients to simple integers.
4
Take the square root of both sides and solve for xx.
1x=20.60x    0.60x=2x    3x=0.60    x=0.20 m\frac{1}{x} = \frac{2}{0.60 - x} \implies 0.60 - x = 2x \implies 3x = 0.60 \implies x = 0.20\text{ m}.
Taking the square root removes the quadratic terms and gives a linear relation for the distance xx from q1q_1.

Key Concept

Electric field superposition and point of zero field intensity between like point charges
Question 72Question

A charged oil droplet of mass 3.2×1015 kg3.2 \times 10^{-15}\text{ kg} remains stationary in a vacuum between two horizontal charged plates where there is a uniform vertical electric field of strength 2.0×104 N C12.0 \times 10^4\text{ N C}^{-1}. Taking g=10 m s2g = 10\text{ m s}^{-2} and the elementary charge e=1.6×1019 Ce = 1.6 \times 10^{-19}\text{ C}, determine the number of excess electrons on the droplet.

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Answer: 10

Answer

The number of excess electrons on the droplet is 10.
The droplet is in mechanical equilibrium under two equal and opposite forces: the downward gravitational force W=mgW = mg and the upward electric force Fe=qEF_e = qE. Setting qE=mgqE = mg gives q=mgE=1.6×1018 Cq = \frac{mg}{E} = 1.6 \times 10^{-18}\text{ C}. By the quantization of charge (q=Neq = Ne), dividing this charge by the elementary charge e=1.6×1019 Ce = 1.6 \times 10^{-19}\text{ C} gives exactly 10 excess electrons.

Step-by-Step Solution

1
Calculate the gravitational force (weight) acting on the droplet.
W=mg=(3.2×1015 kg)×(10 m s2)=3.2×1014 NW = mg = (3.2 \times 10^{-15}\text{ kg}) \times (10\text{ m s}^{-2}) = 3.2 \times 10^{-14}\text{ N}.
For stationary equilibrium, weight provides the downward vertical force.
2
Apply the equilibrium condition to find the electric force.
Fe=W=3.2×1014 NF_e = W = 3.2 \times 10^{-14}\text{ N}.
The net vertical force must be zero for the droplet to remain suspended.
3
Determine the charge qq using Fe=qEF_e = qE.
q=FeE=3.2×1014 N2.0×104 N C1=1.6×1018 Cq = \frac{F_e}{E} = \frac{3.2 \times 10^{-14}\text{ N}}{2.0 \times 10^4\text{ N C}^{-1}} = 1.6 \times 10^{-18}\text{ C}.
Electric field strength relates force and charge.
4
Calculate the number of elementary charges using charge quantization q=Neq = Ne.
N=qe=1.6×1018 C1.6×1019 C=10N = \frac{q}{e} = \frac{1.6 \times 10^{-18}\text{ C}}{1.6 \times 10^{-19}\text{ C}} = 10.
Electric charge exists in discrete integer multiples of the elementary charge ee.

Key Concept

Equilibrium between electrostatic and gravitational forces combined with charge quantization.
Question 73Question

A step-down transformer connected to a 240 V240\text{ V} AC mains supply operates a 12 V,48 W12\text{ V}, 48\text{ W} lamp at its normal brightness rating. If the efficiency of the transformer is 80%80\%, what is the electric current drawn by the primary winding from the mains supply?

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Answer: 0.25 A0.25\text{ A}

Answer

0.25 A0.25\text{ A}
The output power delivered to the lamp is 48 W48\text{ W}. Accounting for the transformer's 80%80\% efficiency, the input power required at the primary winding is 48 W0.80=60 W\frac{48\text{ W}}{0.80} = 60\text{ W}. Since the primary voltage is 240 V240\text{ V}, the primary current drawn is Ip=60 W240 V=0.25 AI_p = \frac{60\text{ W}}{240\text{ V}} = 0.25\text{ A}.

Step-by-Step Solution

1
Determine the power output at the secondary winding
Ps=48 WP_s = 48\text{ W}
The lamp operates at its normal rating, so secondary power equals the lamp rating.
2
Calculate the required power input to the primary winding using transformer efficiency
Pp=Psη=48 W0.80=60 WP_p = \frac{P_s}{\eta} = \frac{48\text{ W}}{0.80} = 60\text{ W}
Efficiency is defined as η=PsPp\eta = \frac{P_s}{P_p}, meaning primary input power must exceed secondary output power due to losses.
3
Compute the primary current drawn from the supply
Ip=PpVp=60 W240 V=0.25 AI_p = \frac{P_p}{V_p} = \frac{60\text{ W}}{240\text{ V}} = 0.25\text{ A}
Power in an AC primary circuit is given by Pp=VpIpP_p = V_p I_p assuming a purely resistive secondary load.

Key Concept

Transformer Efficiency and Power Transfer in Electromagnetic Induction
Question 74Question

A series alternating current (AC) circuit consists of a resistor of resistance 6 Ω6\ \Omega and an inductor with inductive reactance 8 Ω8\ \Omega. What is the total impedance of the circuit?

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Answer: 10 Ω10\ \Omega

Answer

The total impedance of the circuit is 10 Ω10\ \Omega.
In a series RL alternating current circuit, total impedance ZZ combines resistance RR and inductive reactance XLX_L as perpendicular vector components. Using Z=R2+XL2Z = \sqrt{R^2 + X_L^2}, substituting R=6 ΩR = 6\ \Omega and XL=8 ΩX_L = 8\ \Omega gives Z=62+82=100=10 ΩZ = \sqrt{6^2 + 8^2} = \sqrt{100} = 10\ \Omega.

Step-by-Step Solution

1
Identify the given values for resistance and inductive reactance.
R=6 ΩR = 6\ \Omega and XL=8 ΩX_L = 8\ \Omega.
These are the resistive and reactive opposition components in the series RL circuit.
2
Apply the impedance formula for a series RL circuit.
Z=R2+XL2Z = \sqrt{R^2 + X_L^2}
Voltage across a resistor and an inductor are 9090^\circ out of phase, requiring vector/phasor addition to determine total impedance.
3
Calculate the magnitude of total impedance.
Z=62+82=36+64=100=10 ΩZ = \sqrt{6^2 + 8^2} = \sqrt{36 + 64} = \sqrt{100} = 10\ \Omega.
Evaluating the square root yields the net opposing effect to AC current flow.

Key Concept

Impedance in a Series RL Circuit
Question 75Question

An alternating current supply is connected in series with a resistor of resistance 12 Ω12\ \Omega and an inductor of inductive reactance 5 Ω5\ \Omega. What is the total impedance of the circuit?

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Answer: 13 Ω13\ \Omega

Answer

13 Ω13\ \Omega
In a series R-L alternating current circuit, the voltage across the resistor is in phase with the current, while the voltage across the inductor leads the current by 9090^\circ. Consequently, resistance and inductive reactance combine vectorially. The total impedance is Z=R2+XL2=122+52=169=13 ΩZ = \sqrt{R^2 + X_L^2} = \sqrt{12^2 + 5^2} = \sqrt{169} = 13\ \Omega.

Step-by-Step Solution

1
Identify the given values
Resistance R=12 ΩR = 12\ \Omega, inductive reactance XL=5 ΩX_L = 5\ \Omega
These are the given parameters of the series R-L circuit.
2
Apply the total impedance formula for a series R-L AC circuit
Z=R2+XL2Z = \sqrt{R^2 + X_L^2}
In an AC circuit, resistance and reactance are perpendicular vectors (9090^\circ out of phase).
3
Substitute the given values and calculate the result
Z=122+52=144+25=169=13 ΩZ = \sqrt{12^2 + 5^2} = \sqrt{144 + 25} = \sqrt{169} = 13\ \Omega
Evaluating the square root yields the total opposition to alternating current.

Key Concept

Impedance of Series AC Circuits
Estimated Time:45s
Question 76Question

A series alternating current circuit comprises a resistor with resistance 30 Ω30\ \Omega, an inductor with inductive reactance 80 Ω80\ \Omega, and a capacitor with capacitive reactance 40 Ω40\ \Omega. What is the total impedance of the circuit?

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Answer: 50 Ω50\ \Omega

Answer

The impedance of the circuit is 50 Ω50\ \Omega.
The impedance ZZ of a series RLC circuit is calculated using the formula Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}. Substituting the given values R=30 ΩR = 30\ \Omega, XL=80 ΩX_L = 80\ \Omega, and XC=40 ΩX_C = 40\ \Omega yields Z=302+(8040)2=900+1600=50 ΩZ = \sqrt{30^2 + (80 - 40)^2} = \sqrt{900 + 1600} = 50\ \Omega.

Step-by-Step Solution

1
Calculate the net reactance (XnetX_{net})
Xnet=XLXC=80 Ω40 Ω=40 ΩX_{net} = X_L - X_C = 80\ \Omega - 40\ \Omega = 40\ \Omega
Inductive and capacitive reactances are 180180^\circ out of phase in a series AC circuit.
2
Apply the series impedance formula
Z=R2+Xnet2=302+402=900+1600=2500=50 ΩZ = \sqrt{R^2 + X_{net}^2} = \sqrt{30^2 + 40^2} = \sqrt{900 + 1600} = \sqrt{2500} = 50\ \Omega
Resistance and net reactance act at 9090^\circ phase to each other, requiring the Pythagorean relation.

Key Concept

Impedance of a Series RLC Circuit
Question 77Question

A capacitor of capacitance 50 μF50\ \mu\text{F} is connected across an alternating current (AC) source operating at a frequency of 100π Hz\frac{100}{\pi}\ \text{Hz}. What is the capacitive reactance of the capacitor?

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Answer: 100

Answer

The capacitive reactance of the capacitor is 100 Ω100\ \Omega.
Capacitive reactance XCX_C is given by the formula XC=12πfCX_C = \frac{1}{2\pi f C}. Substituting C=50×106 FC = 50 \times 10^{-6}\ \text{F} and f=100π Hzf = \frac{100}{\pi}\ \text{Hz} into the formula yields XC=12π(100/π)(50×106)=1102=100 ΩX_C = \frac{1}{2\pi (100/\pi) (50 \times 10^{-6})} = \frac{1}{10^{-2}} = 100\ \Omega.

Step-by-Step Solution

1
Convert capacitance to farads and state all given values
C=50×106 FC = 50 \times 10^{-6}\ \text{F} and f=100π Hzf = \frac{100}{\pi}\ \text{Hz}
Calculations require standard SI base units.
2
Apply the formula for capacitive reactance
XC=12πfCX_C = \frac{1}{2\pi f C}
Capacitive reactance measures the opposition offered by a capacitor to alternating current.
3
Substitute the values and calculate the result
XC=12π100π(50×106)=110,000×106=100 ΩX_C = \frac{1}{2\pi \cdot \frac{100}{\pi} \cdot (50 \times 10^{-6})} = \frac{1}{10,000 \times 10^{-6}} = 100\ \Omega
The factor π\pi cancels out directly, making the arithmetic simple.

Key Concept

Capacitive Reactance in AC Circuits
Question 78Question

An alternating current (AC) series circuit contains a resistor, an inductor, and a capacitor. The root-mean-square (RMS) potential differences measured across the resistor, inductor, and capacitor are 80 V80\text{ V}, 110 V110\text{ V}, and 50 V50\text{ V}, respectively. What is the total supply voltage across the circuit in volts?

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Answer: 100

Answer

The total supply voltage across the series AC circuit is 100 V100\text{ V}.
In a series alternating current circuit, the voltages across the resistor, inductor, and capacitor are not in phase. The resistor voltage is in phase with the current, whereas inductor voltage leads by 9090^\circ and capacitor voltage lags by 9090^\circ. The total voltage is calculated using vector addition: V=VR2+(VLVC)2V = \sqrt{V_R^2 + (V_L - V_C)^2}. Substituting the given values gives V=802+(11050)2=802+602=6400+3600=100 VV = \sqrt{80^2 + (110 - 50)^2} = \sqrt{80^2 + 60^2} = \sqrt{6400 + 3600} = 100\text{ V}.

Step-by-Step Solution

1
Identify the RMS potential differences across each component.
VR=80 VV_R = 80\text{ V}, VL=110 VV_L = 110\text{ V}, and VC=50 VV_C = 50\text{ V}.
In a series AC circuit, voltages across reactive components are out of phase with the resistor voltage.
2
Calculate the net reactive voltage difference between the inductor and capacitor.
VLVC=110 V50 V=60 VV_L - V_C = 110\text{ V} - 50\text{ V} = 60\text{ V}.
Inductive voltage leads current by 9090^\circ while capacitive voltage lags current by 9090^\circ, making them 180180^\circ out of phase with each other.
3
Determine total supply voltage using vector (phasor) addition.
V=VR2+(VLVC)2=802+602=6400+3600=10000=100 VV = \sqrt{V_R^2 + (V_L - V_C)^2} = \sqrt{80^2 + 60^2} = \sqrt{6400 + 3600} = \sqrt{10000} = 100\text{ V}.
The resistive voltage and net reactive voltage are perpendicular (9090^\circ phase angle difference).

Key Concept

Phasor Addition of Voltages in a Series AC Circuit
Question 79Question

An insulated neutral conductor gains 5.0×10135.0 \times 10^{13} electrons during a electrostatic charging process. Given that the magnitude of the elementary charge is e=1.6×1019 Ce = 1.6 \times 10^{-19}\text{ C}, what is the magnitude of the net charge acquired by the conductor in microcoulombs (μC\mu\text{C})?

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Answer: 8

Answer

The magnitude of the net electric charge acquired by the conductor is 8.0 μC8.0\ \mu\text{C}.
According to the principle of charge quantization, the total magnitude of charge QQ acquired by gaining nn electrons is given by Q=neQ = n e. Substituting n=5.0×1013n = 5.0 \times 10^{13} and e=1.6×1019 Ce = 1.6 \times 10^{-19}\text{ C} gives Q=8.0×106 CQ = 8.0 \times 10^{-6}\text{ C}. Expressed in microcoulombs, 8.0×106 C=8.0 μC8.0 \times 10^{-6}\text{ C} = 8.0\ \mu\text{C}.

Step-by-Step Solution

1
Apply the principle of quantization of electric charge formula
Formula Q=neQ = n e established
Electric charge is quantized and exists in integer multiples of the elementary charge.
2
Multiply the number of electrons by the elementary charge value
Q=8.0×106 CQ = 8.0 \times 10^{-6}\text{ C}
Calculates total electrostatic charge in base SI units.
3
Convert the value from Coulombs to microcoulombs
8.0 μC8.0\ \mu\text{C}
The unit 1 μC1\ \mu\text{C} equals 106 C10^{-6}\text{ C}.

Key Concept

Quantization of Electric Charge
Question 80Question

A small charged sphere of mass 2.0×104 kg2.0 \times 10^{-4}\text{ kg} carrying a positive charge of +4.0×108 C+4.0 \times 10^{-8}\text{ C} is suspended by a light insulating string between two vertical parallel plates. When a uniform horizontal electric field of magnitude EE is applied between the plates, the string deflects and comes to equilibrium at an angle of 4545^\circ to the vertical. Taking the acceleration due to gravity g=10 ms2g = 10\text{ m}\cdot\text{s}^{-2}, calculate the magnitude of the electric field intensity EE in NC1\text{N}\cdot\text{C}^{-1}.

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Answer: 50000

Answer

The magnitude of the electric field intensity is 50000 NC150000\text{ N}\cdot\text{C}^{-1} (or 5.0×104 NC15.0 \times 10^4\text{ N}\cdot\text{C}^{-1}).
In electrostatic equilibrium, the sphere experiences three forces: weight (mgmg) vertically downward, electrostatic force (qEqE) horizontally, and tension (TT) along the thread at 4545^\circ to the vertical. Balancing components gives Tsin45=qET \sin 45^\circ = qE and Tcos45=mgT \cos 45^\circ = mg. Dividing these yields tan45=qEmg=1\tan 45^\circ = \frac{qE}{mg} = 1, which gives qE=mgqE = mg. Substituting the given values gives E=2.0×1034.0×108=50000 NC1E = \frac{2.0 \times 10^{-3}}{4.0 \times 10^{-8}} = 50000\text{ N}\cdot\text{C}^{-1}.

Step-by-Step Solution

1
Calculate the weight of the charged sphere.
W=mg=(2.0×104 kg)(10 ms2)=2.0×103 NW = mg = (2.0 \times 10^{-4}\text{ kg})(10\text{ m}\cdot\text{s}^{-2}) = 2.0 \times 10^{-3}\text{ N}.
The weight provides the downward vertical force in equilibrium.
2
Relate the electrostatic force to the weight using the angle of deflection.
tan(45)=FeW    1=Fe2.0×103 N    Fe=2.0×103 N\tan(45^\circ) = \frac{F_e}{W} \implies 1 = \frac{F_e}{2.0 \times 10^{-3}\text{ N}} \implies F_e = 2.0 \times 10^{-3}\text{ N}.
In electrostatic equilibrium, the ratio of the horizontal force to the vertical force equals the tangent of the angle with the vertical.
3
Calculate the electric field strength EE using Fe=qEF_e = qE.
E=Feq=2.0×103 N4.0×108 C=50000 NC1E = \frac{F_e}{q} = \frac{2.0 \times 10^{-3}\text{ N}}{4.0 \times 10^{-8}\text{ C}} = 50000\text{ N}\cdot\text{C}^{-1}.
The electric field intensity is the electric force per unit charge.

Key Concept

Equilibrium of a charged body in a uniform electric field
Estimated Time:2m 0s
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