Electricity and Magnetism

198 questions

Question 81Question

Two point charges, q1=+4.0×108 Cq_1 = +4.0 \times 10^{-8}\text{ C} and q2=9.0×108 Cq_2 = -9.0 \times 10^{-8}\text{ C}, are fixed in a vacuum at a distance of 0.50 m0.50\text{ m} apart. A third point charge q3=+2.0×108 Cq_3 = +2.0 \times 10^{-8}\text{ C} is placed along the line passing through q1q_1 and q2q_2 such that the net electrostatic force acting on it is zero. What is the distance of q3q_3 from q1q_1?

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Answer: 1.00 m1.00\text{ m}

Answer

The distance of the third charge from q1q_1 is 1.00 m1.00\text{ m} (located on the side of q1q_1 opposite to q2q_2).
The correct distance of 1.00 m1.00\text{ m} is determined by recognizing that zero net force on a test charge q3q_3 occurs outside the opposite charges q1q_1 and q2q_2, specifically on the side of the smaller charge q1q_1. Equating electrostatic forces gives 4d2=9(d+0.50)2\frac{4}{d^2} = \frac{9}{(d+0.50)^2}, which yields d=1.00 md = 1.00\text{ m}.

Step-by-Step Solution

1
Determine the equilibrium region for the third charge.
Because q1=+4.0×108 Cq_1 = +4.0 \times 10^{-8}\text{ C} and q2=9.0×108 Cq_2 = -9.0 \times 10^{-8}\text{ C} have opposite charges, electrostatic forces on q3q_3 point in opposite directions only outside the segment connecting them. To balance the forces, q3q_3 must be closer to the smaller magnitude charge q1q_1, placing it at distance dd to the left of q1q_1.
Between two opposite charges, the force from the positive charge and the force from the negative charge act in the same direction, so net zero force is impossible between them.
2
Set up Coulomb's Law equilibrium equation.
kq1q3d2=kq2q3(d+0.50)2    4.0×108d2=9.0×108(d+0.50)2\frac{k |q_1 q_3|}{d^2} = \frac{k |q_2 q_3|}{(d + 0.50)^2} \implies \frac{4.0 \times 10^{-8}}{d^2} = \frac{9.0 \times 10^{-8}}{(d + 0.50)^2}
Equilibrium requires the force magnitude exerted by q1q_1 on q3q_3 to equal the force magnitude exerted by q2q_2 on q3q_3.
3
Solve the equation for distance dd.
4d2=9(d+0.50)2    2d=3d+0.50    2(d+0.50)=3d    d=1.00 m\frac{4}{d^2} = \frac{9}{(d + 0.50)^2} \implies \frac{2}{d} = \frac{3}{d + 0.50} \implies 2(d + 0.50) = 3d \implies d = 1.00\text{ m}.
Taking the square root of both sides simplifies the inverse-square relation to a solvable linear relation.

Key Concept

Electrostatic equilibrium and vector force cancellation for point charges
Question 82Question

Two point charges produce mutually perpendicular electric fields at a point PP in a vacuum. If the magnitudes of the electric field intensities at PP due to the charges individually are 30 N C130\text{ N C}^{-1} and 40 N C140\text{ N C}^{-1}, what is the magnitude of the net electric field intensity at point PP?

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Answer: 50 N C150\text{ N C}^{-1}

Answer

The magnitude of the net electric field intensity at point PP is 50 N C150\text{ N C}^{-1}.
Because electric field intensity is a vector quantity, two mutually perpendicular electric fields E1=30 N C1E_1 = 30\text{ N C}^{-1} and E2=40 N C1E_2 = 40\text{ N C}^{-1} combine vectorially according to Enet=E12+E22=302+402=50 N C1E_{\text{net}} = \sqrt{E_1^2 + E_2^2} = \sqrt{30^2 + 40^2} = 50\text{ N C}^{-1}.

Step-by-Step Solution

1
Identify the vector nature and orientation of the given electric fields.
The two component fields E1=30 N C1E_1 = 30\text{ N C}^{-1} and E2=40 N C1E_2 = 40\text{ N C}^{-1} are perpendicular to each other (θ=90\theta = 90^\circ).
Electric field intensity is a vector quantity, so perpendicular vectors must be combined using vector addition.
2
Apply the Pythagorean theorem to calculate the resultant vector magnitude.
Enet=E12+E22=302+402=900+1600=2500=50 N C1E_{\text{net}} = \sqrt{E_1^2 + E_2^2} = \sqrt{30^2 + 40^2} = \sqrt{900 + 1600} = \sqrt{2500} = 50\text{ N C}^{-1}.
When two vectors meet at a right angle, the magnitude of their resultant is the hypotenuse of the right-angled triangle formed by the vector components.

Key Concept

Vector Addition of Electric Fields (Superposition Principle)
Estimated Time:1m 0s
Question 83Question

Two identical point charges, q1=+5.0×106 Cq_1 = +5.0 \times 10^{-6}\text{ C} and q2=+5.0×106 Cq_2 = +5.0 \times 10^{-6}\text{ C}, are fixed in a vacuum at Cartesian coordinates (0 m,3.0 m)(0\text{ m}, 3.0\text{ m}) and (0 m,3.0 m)(0\text{ m}, -3.0\text{ m}), respectively. A third point charge q3=+2.0×106 Cq_3 = +2.0 \times 10^{-6}\text{ C} is placed on the x-axis at (4.0 m,0 m)(4.0\text{ m}, 0\text{ m}). Taking Coulomb's constant k=9.0×109 N m2 C2k = 9.0 \times 10^9\text{ N m}^2\text{ C}^{-2}, what is the magnitude of the net electrostatic force exerted on q3q_3?

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Answer: 5.76×103 N5.76 \times 10^{-3}\text{ N}

Answer

The magnitude of the net electrostatic force exerted on q3q_3 is 5.76×103 N5.76 \times 10^{-3}\text{ N}.
Each charge exerts a repulsive force of magnitude 3.60×103 N3.60 \times 10^{-3}\text{ N} along the line connecting it to the test charge at (4.0 m,0 m)(4.0\text{ m}, 0\text{ m}). Because of symmetry, the y-components of the two forces cancel out completely while their x-components add constructively. Multiplying the individual force magnitude by the cosine of the angle with the x-axis (cosθ=0.8\cos\theta = 0.8) and doubling for both charges gives a net force of 5.76×103 N5.76 \times 10^{-3}\text{ N}.

Step-by-Step Solution

1
Calculate the straight-line distance rr from q1q_1 (or q2q_2) to q3q_3.
r=(4.00)2+(03.0)2=16+9=5.0 mr = \sqrt{(4.0 - 0)^2 + (0 - 3.0)^2} = \sqrt{16 + 9} = 5.0\text{ m}.
Coulomb's Law requires the straight-line separation distance between interacting point charges.
2
Calculate the magnitude of the electrostatic force F1F_1 exerted on q3q_3 by q1q_1.
F1=kq1q3r2=(9.0×109)(5.0×106)(2.0×106)5.02=9.0×10225=3.60×103 NF_1 = \frac{k \cdot q_1 \cdot q_3}{r^2} = \frac{(9.0 \times 10^9) \cdot (5.0 \times 10^{-6}) \cdot (2.0 \times 10^{-6})}{5.0^2} = \frac{9.0 \times 10^{-2}}{25} = 3.60 \times 10^{-3}\text{ N}.
By symmetry, the force magnitude F2F_2 from q2q_2 on q3q_3 is also equal to 3.60×103 N3.60 \times 10^{-3}\text{ N}.
3
Determine the vector components of the forces along the axes.
The cosine of the angle θ\theta with the positive x-axis is cosθ=4.05.0=0.8\cos\theta = \frac{4.0}{5.0} = 0.8. The sine is sinθ=3.05.0=0.6\sin\theta = \frac{3.0}{5.0} = 0.6. The vertical y-components are equal in magnitude and opposite in direction (F1y=F2yF_{1y} = -F_{2y}), canceling to zero.
Forces are vector quantities; symmetrically placed identical charges produce opposing vertical components and reinforcing horizontal components.
4
Sum the horizontal x-components to obtain the net force.
Fnet=F1x+F2x=2F1cosθ=2(3.60×103 N)0.8=5.76×103 NF_{\text{net}} = F_{1x} + F_{2x} = 2 \cdot F_1 \cos\theta = 2 \cdot (3.60 \times 10^{-3}\text{ N}) \cdot 0.8 = 5.76 \times 10^{-3}\text{ N}.
Both x-components point along the positive x-axis, so their magnitudes add directly.

Key Concept

Vector superposition of electric forces
Question 84Question

Three point charges q1=+2.0×106 Cq_1 = +2.0 \times 10^{-6}\text{ C}, q2=+2.0×106 Cq_2 = +2.0 \times 10^{-6}\text{ C}, and q3=4.0×106 Cq_3 = -4.0 \times 10^{-6}\text{ C} are placed along a straight line at positions x=0 mx = 0\text{ m}, x=0.30 mx = 0.30\text{ m}, and x=0.60 mx = 0.60\text{ m}, respectively. Taking Coulomb's constant k=9.0×109 N m2 C2k = 9.0 \times 10^9\text{ N m}^2\text{ C}^{-2}, calculate the magnitude of the net electrostatic force acting on charge q2q_2 in newtons.

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Answer: 1.2

Answer

The magnitude of the net electrostatic force acting on charge q2q_2 is 1.20 N1.20\text{ N}.
The force exerted on q2q_2 by q1q_1 is repulsive (0.40 N0.40\text{ N} directed to the right) because both charges are positive. The force exerted on q2q_2 by q3q_3 is attractive (0.80 N0.80\text{ N} directed to the right) because q2q_2 is positive and q3q_3 is negative. Since both component forces act in the same direction, the total net force magnitude is 0.40 N+0.80 N=1.20 N0.40\text{ N} + 0.80\text{ N} = 1.20\text{ N}.

Step-by-Step Solution

1
Calculate the repulsive force exerted by q1q_1 on q2q_2
F12=0.40 NF_{12} = 0.40\text{ N} pointing to the right
Like charges repel each other, so q1q_1 pushes q2q_2 away along the +x+x-axis.
2
Calculate the attractive force exerted by q3q_3 on q2q_2
F32=0.80 NF_{32} = 0.80\text{ N} pointing to the right
Unlike charges attract each other, so q3q_3 pulls q2q_2 towards itself along the +x+x-axis.
3
Sum the component electrostatic forces acting on q2q_2
Fnet=0.40 N+0.80 N=1.20 NF_{\text{net}} = 0.40\text{ N} + 0.80\text{ N} = 1.20\text{ N}
Because both forces act in the exact same direction along the line, their magnitudes add directly.

Key Concept

Coulomb's Law and Principle of Superposition for Electrostatic Forces
Question 85Question

Two capacitors with capacitances of 10 μF10\text{ }\mu\text{F} and 15 μF15\text{ }\mu\text{F} are connected in parallel. What is the equivalent capacitance of the combination in microfarads (μF\mu\text{F})?

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Answer: 25

Answer

The equivalent capacitance of the parallel combination is 25 μF25\text{ }\mu\text{F}.
When capacitors are connected in parallel, the total equivalent capacitance is equal to the direct sum of the individual capacitances: Ceq=C1+C2=10 μF+15 μF=25 μFC_{\text{eq}} = C_1 + C_2 = 10\text{ }\mu\text{F} + 15\text{ }\mu\text{F} = 25\text{ }\mu\text{F}.

Step-by-Step Solution

1
Identify the relationship for parallel capacitors
Ceq=C1+C2C_{\text{eq}} = C_1 + C_2
Capacitors connected in parallel store charge independently across the same potential difference, so their capacitances add directly.
2
Substitute the given values into the formula
Ceq=10 μF+15 μFC_{\text{eq}} = 10\text{ }\mu\text{F} + 15\text{ }\mu\text{F}
The circuit contains two capacitors of 10 μF10\text{ }\mu\text{F} and 15 μF15\text{ }\mu\text{F} in parallel.
3
Calculate the total capacitance
25 μF25\text{ }\mu\text{F}
Simple addition of the two values yields 25 μF25\text{ }\mu\text{F}.

Key Concept

Equivalent Capacitance of Parallel Connected Capacitors
Question 86Question

What is the magnitude of the electric field intensity, in N C1\text{N C}^{-1}, at a point 2.0 m2.0\text{ m} away from a isolated point charge of +4.0×106 C+4.0 \times 10^{-6}\text{ C} in a vacuum? (Take Coulomb's constant k=9.0×109 N m2 C2k = 9.0 \times 10^9\text{ N m}^2\text{ C}^{-2})

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Answer: 9000

Answer

The magnitude of the electric field intensity is 9000 N C19000\text{ N C}^{-1}.
The electric field intensity EE produced by a point charge qq at distance rr is given by E=kqr2E = \frac{kq}{r^2}. Substituting k=9.0×109 N m2 C2k = 9.0 \times 10^9\text{ N m}^2\text{ C}^{-2}, q=4.0×106 Cq = 4.0 \times 10^{-6}\text{ C}, and r=2.0 mr = 2.0\text{ m} yields E=9.0×109×4.0×1064.0=9000 N C1E = \frac{9.0 \times 10^9 \times 4.0 \times 10^{-6}}{4.0} = 9000\text{ N C}^{-1}.

Step-by-Step Solution

1
Identify the given physical quantities and formula
q=4.0×106 Cq = 4.0 \times 10^{-6}\text{ C}, r=2.0 mr = 2.0\text{ m}, k=9.0×109 N m2 C2k = 9.0 \times 10^9\text{ N m}^2\text{ C}^{-2}. Formula: E=kqr2E = \frac{kq}{r^2}
The magnitude of electric field intensity due to a single point charge is given by Coulomb's field law.
2
Substitute the values and calculate the electric field strength
E=9.0×109×4.0×1062.02=360004=9000 N C1E = \frac{9.0 \times 10^9 \times 4.0 \times 10^{-6}}{2.0^2} = \frac{36000}{4} = 9000\text{ N C}^{-1}
Perform basic arithmetic simplification to determine the numerical result.

Key Concept

Electric Field Intensity due to a Point Charge
Question 87Question

Two identical isolated metal spheres, XX and YY, carry initial charges of +q+q and 3q-3q respectively and are separated by a fixed distance rr in a vacuum. The magnitude of the electrostatic force between them is FF. A third identical, uncharged metal sphere ZZ is touched briefly to sphere XX, then touched briefly to sphere YY, and finally placed at the midpoint between spheres XX and YY. What is the magnitude of the net electrostatic force acting on sphere ZZ in terms of FF?

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Answer: 3512F\dfrac{35}{12}F

Answer

The magnitude of the net electrostatic force acting on sphere ZZ is 3512F\dfrac{35}{12}F.
When sphere Z touches sphere X, charge is shared equally so both carry +q2+\frac{q}{2}. Next, when sphere Z touches sphere Y (charge 3q-3q), total charge becomes 5q2-\frac{5q}{2}, dividing equally into 5q4-\frac{5q}{4} for each. At the midpoint (r/2r/2 from each sphere), sphere X (+q2+\frac{q}{2}) attracts sphere Z (5q4-\frac{5q}{4}) towards the left with force 52kq2r2\frac{5}{2}\frac{kq^2}{r^2}. Sphere Y (5q4-\frac{5q}{4}) repels sphere Z (5q4-\frac{5q}{4}) towards the left with force 254kq2r2\frac{25}{4}\frac{kq^2}{r^2}. Adding these co-directional forces yields 354kq2r2\frac{35}{4}\frac{kq^2}{r^2}. Given the initial force F=3kq2r2F = \frac{3kq^2}{r^2}, we substitute kq2r2=F3\frac{kq^2}{r^2} = \frac{F}{3} to obtain 3512F\frac{35}{12}F.

Step-by-Step Solution

1
Determine the initial electrostatic force FF between spheres XX and YY.
F=k(+q)(3q)r2=3kq2r2F = k \frac{|(+q)(-3q)|}{r^2} = \frac{3kq^2}{r^2}, which gives kq2r2=F3\frac{kq^2}{r^2} = \frac{F}{3}.
Coulomb's law defines force as proportional to the product of charges divided by the square of separation distance.
2
Calculate the charges on the spheres after sequential contacts.
When ZZ (00) touches XX (+q+q), charge divides equally: qX=+q2q_X' = +\frac{q}{2} and qZ=+q2q_Z' = +\frac{q}{2}. When ZZ (+q2+\frac{q}{2}) touches YY (3q-3q), the combined charge is +q23q=5q2+\frac{q}{2} - 3q = -\frac{5q}{2}, which divides equally to give qY=5q4q_Y' = -\frac{5q}{4} and qZ=5q4q_Z'' = -\frac{5q}{4}.
Identical conductors share total charge equally upon contact due to conservation of charge and symmetric potential.
3
Determine the forces exerted on sphere ZZ at the midpoint.
Separation distance from ZZ to both XX and YY is r2\frac{r}{2}. Force from XX on ZZ (attractive, pulling towards XX): FZX=k(+q2)(5q4)(r2)2=k5q28r24=52kq2r2F_{ZX} = k \frac{|(+\frac{q}{2})(-\frac{5q}{4})|}{(\frac{r}{2})^2} = k \frac{\frac{5q^2}{8}}{\frac{r^2}{4}} = \frac{5}{2}\frac{kq^2}{r^2}. Force from YY on ZZ (repulsive, pushing away from YY toward XX): FZY=k(5q4)(5q4)(r2)2=k25q216r24=254kq2r2F_{ZY} = k \frac{|(-\frac{5q}{4})(-\frac{5q}{4})|}{(\frac{r}{2})^2} = k \frac{\frac{25q^2}{16}}{\frac{r^2}{4}} = \frac{25}{4}\frac{kq^2}{r^2}.
Opposite charges attract and like charges repel. Midpoint separation distance is r/2r/2.
4
Calculate the net force on ZZ and express it in terms of FF.
Since both forces act in the same direction (towards sphere XX), Fnet=FZX+FZY=(52+254)kq2r2=354kq2r2F_{\text{net}} = F_{ZX} + F_{ZY} = (\frac{5}{2} + \frac{25}{4})\frac{kq^2}{r^2} = \frac{35}{4}\frac{kq^2}{r^2}. Substituting kq2r2=F3\frac{kq^2}{r^2} = \frac{F}{3} yields Fnet=354×F3=3512FF_{\text{net}} = \frac{35}{4} \times \frac{F}{3} = \frac{35}{12}F.
Forces in the same direction add vectorially.

Key Concept

Electrostatic Charge Sharing and Coulomb's Law Vector Superposition
Question 88Question

Two capacitors of capacitances C1=6 μFC_1 = 6\text{ }\mu\text{F} and C2=12 μFC_2 = 12\text{ }\mu\text{F} are connected in series across a 180 V180\text{ V} direct current power supply. After the capacitors are fully charged, the supply is disconnected. A dielectric material of dielectric constant K=4K = 4 is then inserted to completely fill the space between the plates of C1C_1. What is the new potential difference across C1C_1?

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Answer: 30 V30\text{ V}

Answer

30 V30\text{ V}
The initial equivalent capacitance of the series combination is 4 μF4\text{ }\mu\text{F}, which charges each capacitor to 720 μC720\text{ }\mu\text{C}. Because the circuit is disconnected from the battery, charge is conserved. Inserting a dielectric of constant K=4K = 4 increases C1C_1 to 24 μF24\text{ }\mu\text{F}, resulting in a potential difference of V=QC1=720 μC24 μF=30 VV = \frac{Q}{C_1'} = \frac{720\text{ }\mu\text{C}}{24\text{ }\mu\text{F}} = 30\text{ V}.

Step-by-Step Solution

1
Calculate the initial equivalent capacitance of the series network
Ceq=4 μFC_{eq} = 4\text{ }\mu\text{F}
Capacitors in series combine reciprocally: 1Ceq=16+112=312=14 μF1\frac{1}{C_{eq}} = \frac{1}{6} + \frac{1}{12} = \frac{3}{12} = \frac{1}{4}\text{ }\mu\text{F}^{-1}.
2
Determine the charge stored on each capacitor prior to disconnection
Q=720 μCQ = 720\text{ }\mu\text{C}
Total charge supplied by the 180 V180\text{ V} battery is Q=CeqV=4 μF×180 V=720 μCQ = C_{eq} V = 4\text{ }\mu\text{F} \times 180\text{ V} = 720\text{ }\mu\text{C}. In series, each capacitor holds this same charge.
3
Calculate the modified capacitance of C1C_1 after dielectric insertion
C1=24 μFC_1' = 24\text{ }\mu\text{F}
A dielectric of constant K=4K = 4 scales capacitance by KK: C1=K×C1=4×6 μF=24 μFC_1' = K \times C_1 = 4 \times 6\text{ }\mu\text{F} = 24\text{ }\mu\text{F}.
4
Calculate the final potential difference across C1C_1 using charge conservation
V1=30 VV_1' = 30\text{ V}
Because the source is disconnected, charge Q=720 μCQ = 720\text{ }\mu\text{C} on C1C_1 remains constant. Therefore, V1=QC1=720 μC24 μF=30 VV_1' = \frac{Q}{C_1'} = \frac{720\text{ }\mu\text{C}}{24\text{ }\mu\text{F}} = 30\text{ V}.

Key Concept

Effect of dielectrics and charge conservation in disconnected series capacitor circuits
Question 89Question

Two identical positive point charges, each of magnitude q=+2.5×106 Cq = +2.5 \times 10^{-6}\text{ C}, are fixed in a vacuum at a distance of 0.60 m0.60\text{ m} apart. A third point charge q0=+1.0×106 Cq_0 = +1.0 \times 10^{-6}\text{ C} is placed on the perpendicular bisector of the line joining the two fixed charges, at a distance of 0.40 m0.40\text{ m} from their midpoint. Taking Coulomb's constant k=9.0×109 N m2 C2k = 9.0 \times 10^9\text{ N m}^2\text{ C}^{-2}, what is the magnitude of the net electrostatic force acting on the third charge, in newtons?

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Answer: 0.144

Answer

The magnitude of the net electrostatic force acting on the third charge is 0.144 N0.144\text{ N}.
Each fixed charge exerts an equal repulsive electrostatic force of 0.09 N0.09\text{ N} on the third charge. Due to the symmetrical arrangement, the force components perpendicular to the bisector cancel each other out, while the parallel components add together, giving a net force of 2×0.09×0.8=0.144 N2 \times 0.09 \times 0.8 = 0.144\text{ N}.

Step-by-Step Solution

1
Determine the distance from each fixed charge to the third charge
r=0.50 mr = 0.50\text{ m}
The charges form a right-angled triangle with base 0.30 m0.30\text{ m} (half of 0.60 m0.60\text{ m}) and height 0.40 m0.40\text{ m}, yielding a hypotenuse of 0.302+0.402=0.50 m\sqrt{0.30^2 + 0.40^2} = 0.50\text{ m}.
2
Calculate the magnitude of the individual repulsive force from one charge
F=0.09 NF = 0.09\text{ N}
Applying Coulomb's law: F=kqq0r2=9.0×109×2.5×106×1.0×1060.25=0.09 NF = \frac{k q q_0}{r^2} = \frac{9.0 \times 10^9 \times 2.5 \times 10^{-6} \times 1.0 \times 10^{-6}}{0.25} = 0.09\text{ N}.
3
Determine directional component of forces along the perpendicular bisector
cosθ=0.8\cos\theta = 0.8
The directional cosine along the axis of symmetry is the ratio of the adjacent side (0.40 m0.40\text{ m}) to the hypotenuse (0.50 m0.50\text{ m}).
4
Compute the net electrostatic force using vector addition
Fnet=0.144 NF_{\text{net}} = 0.144\text{ N}
Horizontal components cancel by symmetry, so Fnet=2Fcosθ=2×0.09×0.8=0.144 NF_{\text{net}} = 2 F \cos\theta = 2 \times 0.09 \times 0.8 = 0.144\text{ N}.

Key Concept

Vector superposition of Coulombic forces along an axis of symmetry
Question 90Question

A parallel plate air capacitor of capacitance 8.0 μF8.0\text{ }\mu\text{F} is fully charged using a 40.0 V40.0\text{ V} d.c. power supply and then disconnected from the source. A dielectric slab with a relative permittivity of 4.04.0 is subsequently inserted to completely fill the region between the plates. Calculate the magnitude of the decrease in electrostatic energy stored in the capacitor, in microjoules (μJ\mu\text{J}).

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Answer: 4800

Answer

The magnitude of the decrease in stored electrostatic energy is 4800 μJ.
Disconnecting the battery ensures that the charge Q=C0V=320 μCQ = C_0 V = 320\text{ }\mu\text{C} on the plates stays fixed. Inserting the dielectric increases capacitance fourfold to 32.0 μF32.0\text{ }\mu\text{F}. The energy decreases from Ui=6400 μJU_i = 6400\text{ }\mu\text{J} to Uf=Q22Cf=1600 μJU_f = \frac{Q^2}{2C_f} = 1600\text{ }\mu\text{J}, giving a total decrease of 4800 μJ4800\text{ }\mu\text{J}.

Step-by-Step Solution

1
Calculate the initial energy stored in the air capacitor before disconnection.
Initial energy Ui=12C0V2=12×8.0×106 F×(40.0 V)2=6.4×103 J=6400 μJU_i = \frac{1}{2} C_0 V^2 = \frac{1}{2} \times 8.0 \times 10^{-6} \text{ F} \times (40.0 \text{ V})^2 = 6.4 \times 10^{-3} \text{ J} = 6400 \text{ } \mu\text{J}.
The initial state has known capacitance and potential difference.
2
Calculate the new capacitance with the dielectric present.
Final capacitance Cf=KC0=4.0×8.0 μF=32.0 μFC_f = K C_0 = 4.0 \times 8.0 \text{ } \mu\text{F} = 32.0 \text{ } \mu\text{F}.
Inserting a dielectric of constant KK scales the capacitance by KK.
3
Calculate the final stored energy using charge conservation.
Final energy Uf=UiK=6400 μJ4.0=1600 μJU_f = \frac{U_i}{K} = \frac{6400 \text{ } \mu\text{J}}{4.0} = 1600 \text{ } \mu\text{J}.
Disconnection forces the charge QQ to remain fixed, so energy scales inversely with capacitance (U=Q22CU = \frac{Q^2}{2C}).
4
Find the difference between initial and final energy.
\Delta U = 6400 \text{ } \mu\text{J} - 1600 \text{ } \mu\text{J} = 4800 \text{ } \mu\text{J}.
The loss in electrostatic energy represents the work done by the field pulling the dielectric slab into the plates.

Key Concept

Effect of dielectric insertion on stored electrostatic energy under isolated (constant charge) conditions
Estimated Time:2m 0s
Question 91Question

An electric charge of +3.2×1019 C+3.2 \times 10^{-19}\text{ C} is situated in a uniform electric field of strength 5.0×104 N C15.0 \times 10^4\text{ N C}^{-1}. What is the magnitude of the electrostatic force exerted on the charge?

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Answer: 1.6×1014 N1.6 \times 10^{-14}\text{ N}

Answer

The magnitude of the electrostatic force exerted on the charge is 1.6×1014 N1.6 \times 10^{-14}\text{ N}.
The relationship between electric field intensity EE, charge qq, and electrostatic force FF is given by F=qEF = qE. Multiplying +3.2×1019 C+3.2 \times 10^{-19}\text{ C} by 5.0×104 N C15.0 \times 10^4\text{ N C}^{-1} gives 1.6×1014 N1.6 \times 10^{-14}\text{ N}, which correctly expresses the force magnitude in standard notation.

Step-by-Step Solution

1
Identify the given values and formula.
Charge q=3.2×1019 Cq = 3.2 \times 10^{-19}\text{ C}, Electric field strength E=5.0×104 N C1E = 5.0 \times 10^4\text{ N C}^{-1}. Formula: F=qEF = qE.
The force experienced by a charge in an electric field is the product of the charge magnitude and the field strength.
2
Substitute the values into the formula and calculate.
F=(3.2×1019)×(5.0×104)=16.0×1015 N=1.6×1014 NF = (3.2 \times 10^{-19}) \times (5.0 \times 10^4) = 16.0 \times 10^{-15}\text{ N} = 1.6 \times 10^{-14}\text{ N}.
Multiplying the numerical coefficients (3.2×5.0=16.0)(3.2 \times 5.0 = 16.0) and combining the powers of ten (1019×104=1015)(10^{-19} \times 10^4 = 10^{-15}) gives 1.6×1014 N1.6 \times 10^{-14}\text{ N} in standard scientific notation.

Key Concept

Electric Field Intensity and Electrostatic Force (F=qEF = qE)
Question 92Question

A parallel-plate capacitor with air between its plates has a capacitance of 12 μF12\text{ }\mu\text{F}. A dielectric slab of relative permittivity εr=4\varepsilon_r = 4 and thickness t=d3t = \frac{d}{3}, where dd is the total plate separation, is inserted between the plates parallel to them. What is the effective capacitance of the modified capacitor?

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Answer: 16 μF16\text{ }\mu\text{F}

Answer

The effective capacitance of the modified capacitor is 16 μF16\text{ }\mu\text{F}.
Inserting a dielectric slab of thickness t=d/3t = d/3 creates a system equivalent to two series capacitors: an air-filled region of thickness 2d/32d/3 (C1=1.5C0=18 μFC_1 = 1.5 C_0 = 18\text{ }\mu\text{F}) and a dielectric-filled region of thickness d/3d/3 (C2=12C0=144 μFC_2 = 12 C_0 = 144\text{ }\mu\text{F}). Combining them via the series reciprocal formula gives Ceq=18×14418+144=16 μFC_{\text{eq}} = \frac{18 \times 144}{18 + 144} = 16\text{ }\mu\text{F}.

Step-by-Step Solution

1
Model the partially filled capacitor as two capacitors connected in series.
Air layer of thickness d1=dt=23dd_1 = d - t = \frac{2}{3}d forms capacitor C1C_1. Dielectric layer of thickness d2=t=13dd_2 = t = \frac{1}{3}d forms capacitor C2C_2.
Dividing the plate gap vertically into two distinct media creates two capacitive regions sharing the same electric flux path.
2
Calculate the individual capacitances C1C_1 and C2C_2 in terms of initial air capacitance C0=12 μFC_0 = 12\text{ }\mu\text{F}.
C1=ε0A23d=32C0=32(12)=18 μFC_1 = \frac{\varepsilon_0 A}{\frac{2}{3}d} = \frac{3}{2}C_0 = \frac{3}{2}(12) = 18\text{ }\mu\text{F} and C2=εrε0A13d=3εrC0=3(4)(12)=144 μFC_2 = \frac{\varepsilon_r \varepsilon_0 A}{\frac{1}{3}d} = 3 \varepsilon_r C_0 = 3(4)(12) = 144\text{ }\mu\text{F}.
Capacitance is inversely proportional to plate distance and directly proportional to relative permittivity.
3
Calculate the equivalent capacitance CeqC_{\text{eq}} for two series capacitors.
1Ceq=1C1+1C2=118+1144=8+1144=9144=116 μF1    Ceq=16 μF\frac{1}{C_{\text{eq}}} = \frac{1}{C_1} + \frac{1}{C_2} = \frac{1}{18} + \frac{1}{144} = \frac{8 + 1}{144} = \frac{9}{144} = \frac{1}{16}\text{ }\mu\text{F}^{-1} \implies C_{\text{eq}} = 16\text{ }\mu\text{F}.
Capacitors connected in series combine reciprocally.

Key Concept

Partially filled parallel-plate capacitors act as series combinations of distinct capacitive layers.
Estimated Time:3m 0s
Question 93Question

Two capacitors with capacitances of 3.0 μF3.0\text{ }\mu\text{F} and 6.0 μF6.0\text{ }\mu\text{F} are connected in parallel across a direct-current source. What is the equivalent capacitance of this combination?

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Answer: 9.0 μF9.0\text{ }\mu\text{F}

Answer

The equivalent capacitance of the parallel combination is 9.0 μF9.0\text{ }\mu\text{F}.
When capacitors are connected in parallel, each capacitor experiences the full potential difference of the voltage source, and the total charge stored is the sum of individual charges (Qtotal=Q1+Q2Q_{total} = Q_1 + Q_2). Thus, the equivalent capacitance is the direct sum of the individual capacitances: Ceq=3.0 μF+6.0 μF=9.0 μFC_{eq} = 3.0\text{ }\mu\text{F} + 6.0\text{ }\mu\text{F} = 9.0\text{ }\mu\text{F}.

Step-by-Step Solution

1
Identify the combination rule for parallel capacitors.
The total capacitance is given by Ceq=C1+C2C_{eq} = C_1 + C_2.
Capacitors in parallel share the same potential difference, so total charge stored is the sum of individual charges.
2
Substitute the given values into the parallel capacitance formula.
Ceq=3.0 μF+6.0 μF=9.0 μFC_{eq} = 3.0\text{ }\mu\text{F} + 6.0\text{ }\mu\text{F} = 9.0\text{ }\mu\text{F}.
Direct addition yields the total equivalent capacitance.

Key Concept

Parallel Combination of Capacitors
Estimated Time:45s
Question 94Question

Two identical air-filled parallel-plate capacitors, C1C_1 and C2C_2, each of capacitance CC, are connected in series across a direct-current voltage source of potential difference VV. While the circuit remains connected to the voltage source, a dielectric slab of relative permittivity εr=3\varepsilon_r = 3 is fully inserted into C1C_1, completely filling the space between its plates. What is the ratio of the electrostatic energy stored in C1C_1 after inserting the dielectric to the energy stored in C1C_1 before the insertion?

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Answer: 3:43 : 4

Answer

The ratio of the energy stored in the first capacitor after dielectric insertion to before insertion is 3:43 : 4 (or 0.750.75).
Initially, the two identical capacitors divide the total source voltage VV equally, giving V1=V/2V_1 = V/2 and initial energy U1,i=18CV2U_{1,i} = \frac{1}{8} C V^2. When the dielectric of relative permittivity 33 is inserted, the capacitance of the first capacitor becomes 3C3C. In a series circuit connected to a constant voltage source, the total charge becomes Q=CeqV=34CVQ = C_{eq}V = \frac{3}{4}CV, which reduces the voltage across the modified capacitor to V1=Q3C=V4V_1' = \frac{Q}{3C} = \frac{V}{4}. The new stored energy is U1,f=12(3C)(V4)2=332CV2U_{1,f} = \frac{1}{2}(3C)(\frac{V}{4})^2 = \frac{3}{32} C V^2. Dividing U1,fU_{1,f} by U1,iU_{1,i} yields 3/321/8=34\frac{3/32}{1/8} = \frac{3}{4}.

Step-by-Step Solution

1
Calculate initial capacitance and voltage across C1C_1
Initial capacitance C1,i=CC_{1,i} = C. Since C1C_1 and C2C_2 are identical and in series, initial potential difference across C1C_1 is V1,i=V2V_{1,i} = \frac{V}{2}.
Equal capacitors in series divide total voltage equally.
2
Calculate initial electrostatic energy stored in C1C_1
U1,i=12C1,iV1,i2=12C(V2)2=18CV2U_{1,i} = \frac{1}{2} C_{1,i} V_{1,i}^2 = \frac{1}{2} C \left(\frac{V}{2}\right)^2 = \frac{1}{8} C V^2.
Formula for energy stored in a capacitor is U=12CV2U = \frac{1}{2} C V^2.
3
Determine final capacitance of C1C_1 and new voltage division
New capacitance C1,f=εrC=3CC_{1,f} = \varepsilon_r C = 3C. Total equivalent capacitance Ceq=3CC3C+C=34CC_{eq} = \frac{3C \cdot C}{3C + C} = \frac{3}{4} C. Total charge supplied Q=CeqV=34CVQ = C_{eq} V = \frac{3}{4} C V. Final voltage across C1C_1 is V1,f=QC1,f=34CV3C=V4V_{1,f} = \frac{Q}{C_{1,f}} = \frac{\frac{3}{4} C V}{3C} = \frac{V}{4}.
Dielectric increases capacitance by factor εr\varepsilon_r, altering equivalent capacitance and potential distribution in series.
4
Calculate final electrostatic energy in C1C_1 and compute the ratio
U1,f=12(3C)(V4)2=332CV2U_{1,f} = \frac{1}{2} (3C) \left(\frac{V}{4}\right)^2 = \frac{3}{32} C V^2. Ratio U1,fU1,i=332CV218CV2=34\frac{U_{1,f}}{U_{1,i}} = \frac{\frac{3}{32} C V^2}{\frac{1}{8} C V^2} = \frac{3}{4}.
Divide final stored energy by initial stored energy.

Key Concept

Series combination of capacitors with dielectric insertion under constant battery voltage
Question 95Question

Three capacitors, each of capacitance 12 μF12\text{ }\mu\text{F}, are arranged such that two of them are connected in parallel, and this combination is connected in series with the third capacitor. If the entire network is connected across a 20 V20\text{ V} d.c. power supply, what is the total energy stored in the network?

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Answer: 1.6×103 J1.6 \times 10^{-3}\text{ J}

Answer

The total energy stored in the network is 1.6×103 J1.6 \times 10^{-3}\text{ J}.
Combining two 12 μF12\text{ }\mu\text{F} capacitors in parallel gives a parallel capacitance of 24 μF24\text{ }\mu\text{F}. Connecting this combination in series with the third 12 μF12\text{ }\mu\text{F} capacitor results in an equivalent network capacitance of Ceq=24×1224+12=8 μFC_{\text{eq}} = \frac{24 \times 12}{24 + 12} = 8\text{ }\mu\text{F}. Substituting this into the energy formula E=12CeqV2E = \frac{1}{2} C_{\text{eq}} V^2 yields E=12×8×106×400=1.6×103 JE = \frac{1}{2} \times 8 \times 10^{-6} \times 400 = 1.6 \times 10^{-3}\text{ J}.

Step-by-Step Solution

1
Calculate the equivalent capacitance of the parallel branch.
Cp=12 μF+12 μF=24 μFC_p = 12\text{ }\mu\text{F} + 12\text{ }\mu\text{F} = 24\text{ }\mu\text{F}
Capacitors in parallel add directly.
2
Calculate the total equivalent capacitance of the network.
Ceq=Cp×C3Cp+C3=24×1224+12=28836=8 μF=8×106 FC_{\text{eq}} = \frac{C_p \times C_3}{C_p + C_3} = \frac{24 \times 12}{24 + 12} = \frac{288}{36} = 8\text{ }\mu\text{F} = 8 \times 10^{-6}\text{ F}
The parallel combination is connected in series with the third capacitor.
3
Calculate the total electrical energy stored in the combination.
E=12CeqV2=12×(8×106 F)×(20 V)2=4×106×400=1.6×103 JE = \frac{1}{2} C_{\text{eq}} V^2 = \frac{1}{2} \times (8 \times 10^{-6}\text{ F}) \times (20\text{ V})^2 = 4 \times 10^{-6} \times 400 = 1.6 \times 10^{-3}\text{ J}
The formula for energy stored in a capacitor network is E=12CV2E = \frac{1}{2} C V^2.

Key Concept

Mixed capacitor networks and energy storage
Estimated Time:1m 30s
Question 96Question

Two electrostatic forces of magnitude 3.0 N3.0\text{ N} and 4.0 N4.0\text{ N} act on a small test charge at right angles (9090^\circ) to each other. What is the magnitude of the net electrostatic force acting on the charge?

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Answer: 5.0 N5.0\text{ N}

Answer

5.0 N5.0\text{ N}
The net electrostatic force is found by vector addition. Since the two forces are perpendicular (9090^\circ), the magnitude of their resultant is given by F12+F22=3.02+4.02=5.0 N\sqrt{F_1^2 + F_2^2} = \sqrt{3.0^2 + 4.0^2} = 5.0\text{ N}.

Step-by-Step Solution

1
Identify the nature of force as a vector quantity.
Electrostatic forces must be combined using vector addition rather than simple scalar addition.
The forces act at right angles (9090^\circ) to each other.
2
Apply the Pythagorean theorem to calculate the magnitude of the resultant net force FnetF_{\text{net}}.
Fnet=F12+F22=3.02+4.02=9+16=25=5.0 NF_{\text{net}} = \sqrt{F_1^2 + F_2^2} = \sqrt{3.0^2 + 4.0^2} = \sqrt{9 + 16} = \sqrt{25} = 5.0\text{ N}.
For perpendicular vectors, the resultant is the hypotenuse of a right-angled triangle formed by the vector components.

Key Concept

Vector Addition of Electrostatic Forces
Question 97Question

Two point charges, q1=+2.0×106 Cq_1 = +2.0 \times 10^{-6}\text{ C} and q2=2.0×106 Cq_2 = -2.0 \times 10^{-6}\text{ C}, are fixed in a vacuum separated by a distance of 0.20 m0.20\text{ m}. What is the magnitude of the net electric field intensity at the midpoint along the line joining the two charges? (Take Coulomb's constant k=9.0×109 N m2 C2k = 9.0 \times 10^9\text{ N m}^2\text{ C}^{-2})

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Answer: 3.6×106 N C13.6 \times 10^6\text{ N C}^{-1}

Answer

3.6×106 N C13.6 \times 10^6\text{ N C}^{-1}
The correct answer is 3.6×106 N C13.6 \times 10^6\text{ N C}^{-1}. At the midpoint (r=0.10 mr = 0.10\text{ m}), the electric field due to the positive charge points towards the negative charge, and the field due to the negative charge also points towards the negative charge. Summing both equal field magnitudes of 1.8×106 N C11.8 \times 10^6\text{ N C}^{-1} yields 3.6×106 N C13.6 \times 10^6\text{ N C}^{-1}.

Step-by-Step Solution

1
Determine the distance from each point charge to the midpoint.
The distance r=0.20 m2=0.10 mr = \frac{0.20\text{ m}}{2} = 0.10\text{ m}.
The midpoint divides the total separation distance equally.
2
Calculate the magnitude of the electric field intensity E1E_1 created by the positive charge q1q_1 at the midpoint.
E1=kq1r2=9.0×109×2.0×106(0.10)2=1.8×106 N C1E_1 = \frac{k |q_1|}{r^2} = \frac{9.0 \times 10^9 \times 2.0 \times 10^{-6}}{(0.10)^2} = 1.8 \times 10^6\text{ N C}^{-1} directed away from q1q_1 (towards q2q_2).
Electric field vectors point away from positive charges.
3
Calculate the magnitude of the electric field intensity E2E_2 created by the negative charge q2q_2 at the midpoint.
E2=kq2r2=9.0×109×2.0×106(0.10)2=1.8×106 N C1E_2 = \frac{k |q_2|}{r^2} = \frac{9.0 \times 10^9 \times 2.0 \times 10^{-6}}{(0.10)^2} = 1.8 \times 10^6\text{ N C}^{-1} directed towards q2q_2.
Electric field vectors point towards negative charges.
4
Combine the electric field vectors vectorially to find the net field intensity.
Enet=E1+E2=1.8×106+1.8×106=3.6×106 N C1E_{\text{net}} = E_1 + E_2 = 1.8 \times 10^6 + 1.8 \times 10^6 = 3.6 \times 10^6\text{ N C}^{-1}.
Because both E1E_1 and E2E_2 point in the exact same direction (towards q2q_2), their magnitudes add directly.

Key Concept

Superposition Principle of Electric Fields
Question 98Question

In an electric circuit, two capacitors C1=12 μFC_1 = 12\text{ }\mu\text{F} and C2=6 μFC_2 = 6\text{ }\mu\text{F} are connected in series. This series combination is then connected in parallel with a third capacitor C3C_3 of unknown value. When a direct-current potential difference of 100 V100\text{ V} is applied across the entire network, the total electrostatic energy stored in the circuit is 100 mJ100\text{ mJ}. What is the capacitance of C3C_3 in microfarads (μF\mu\text{F})?

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Answer: 16

Answer

The capacitance of C3C_3 is 16 μF16\text{ }\mu\text{F}.
First, the series combination of 12 μF12\text{ }\mu\text{F} and 6 μF6\text{ }\mu\text{F} yields an equivalent branch capacitance of 4 μF4\text{ }\mu\text{F}. Second, using E=12CeqV2E = \frac{1}{2} C_{eq} V^2 with E=0.100 JE = 0.100\text{ J} and V=100 VV = 100\text{ V} gives a total circuit equivalent capacitance of 20 μF20\text{ }\mu\text{F}. Finally, subtracting the branch capacitance from the total parallel equivalent capacitance gives C3=20 μF4 μF=16 μFC_3 = 20\text{ }\mu\text{F} - 4\text{ }\mu\text{F} = 16\text{ }\mu\text{F}.

Step-by-Step Solution

1
Calculate the effective capacitance of the series branch containing C1C_1 and C2C_2
C12=4 μFC_{12} = 4\text{ }\mu\text{F}
Capacitors in series combine reciprocally: 1C12=1C1+1C2=112+16=312    C12=4 μF\frac{1}{C_{12}} = \frac{1}{C_1} + \frac{1}{C_2} = \frac{1}{12} + \frac{1}{6} = \frac{3}{12} \implies C_{12} = 4\text{ }\mu\text{F}.
2
Determine the total equivalent capacitance CeqC_{eq} of the circuit using the given stored energy and voltage
Ceq=20 μFC_{eq} = 20\text{ }\mu\text{F}
Energy stored in a capacitor network is E=12CeqV2E = \frac{1}{2} C_{eq} V^2. Rearranging gives Ceq=2EV2=2×0.100 J(100 V)2=20×106 F=20 μFC_{eq} = \frac{2E}{V^2} = \frac{2 \times 0.100\text{ J}}{(100\text{ V})^2} = 20 \times 10^{-6}\text{ F} = 20\text{ }\mu\text{F}.
3
Calculate the unknown capacitance C3C_3 from the parallel combination formula
C3=16 μFC_3 = 16\text{ }\mu\text{F}
Because the branch C12C_{12} and C3C_3 are in parallel, Ceq=C12+C3    20 μF=4 μF+C3    C3=16 μFC_{eq} = C_{12} + C_3 \implies 20\text{ }\mu\text{F} = 4\text{ }\mu\text{F} + C_3 \implies C_3 = 16\text{ }\mu\text{F}.

Key Concept

Series and parallel combinations of capacitors combined with electrostatic energy storage
Estimated Time:2m 0s
Question 99Question

A neutral insulated conductor loses 5.0×10135.0 \times 10^{13} electrons during an electrostatics experiment. What is the magnitude of the net electric charge, in microcoulombs (μC\mu\text{C}), acquired by the conductor? (Take elementary charge e=1.6×1019 Ce = 1.6 \times 10^{-19}\text{ C})

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Answer: 8

Answer

The magnitude of the net electric charge acquired by the conductor is 8 μC8\text{ }\mu\text{C}.
According to the principle of charge quantization, the total electric charge QQ is calculated using Q=neQ = n e. Multiplying 5.0×10135.0 \times 10^{13} electrons by 1.6×1019 C1.6 \times 10^{-19}\text{ C} yields 8.0×106 C8.0 \times 10^{-6}\text{ C}, which converts to 8 μC8\text{ }\mu\text{C}.

Step-by-Step Solution

1
Identify the relevant formula for quantization of charge.
The net charge acquired is given by Q=neQ = n e.
Electric charge is quantized, so the total charge magnitude equals the number of transferred electrons multiplied by the magnitude of charge on a single electron.
2
Calculate the magnitude of charge in Coulombs.
Q=(5.0×1013)×(1.6×1019 C)=8.0×106 CQ = (5.0 \times 10^{13}) \times (1.6 \times 10^{-19}\text{ C}) = 8.0 \times 10^{-6}\text{ C}.
Multiplying the quantity of removed electrons by the elementary charge gives total charge in Coulombs.
3
Convert the calculated value from Coulombs to microcoulombs.
8.0×106 C=8 μC8.0 \times 10^{-6}\text{ C} = 8\text{ }\mu\text{C}.
Since 1 μC=106 C1\text{ }\mu\text{C} = 10^{-6}\text{ C}, dividing 8.0×1068.0 \times 10^{-6} by 10610^{-6} yields 8.

Key Concept

Quantization of Electric Charge
Question 100Question

A 5.0 μF5.0\text{ }\mu\text{F} parallel-plate capacitor is connected across a potential difference of 20.0 V20.0\text{ V}. What is the magnitude of the electric charge stored on either plate of the capacitor, in microcoulombs (μC\mu\text{C})?

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Answer: 100

Answer

The magnitude of the electric charge stored on either plate of the capacitor is 100.0 μC100.0\text{ }\mu\text{C}.
Using the capacitor charge equation Q=C×VQ = C \times V, substituting C=5.0 μFC = 5.0\text{ }\mu\text{F} and V=20.0 VV = 20.0\text{ V} yields Q=5.0×20.0=100.0 μCQ = 5.0 \times 20.0 = 100.0\text{ }\mu\text{C}.

Step-by-Step Solution

1
Identify the given physical quantities and the formula for electric charge on a capacitor.
Capacitance C=5.0 μFC = 5.0\text{ }\mu\text{F}, voltage V=20.0 VV = 20.0\text{ V}. Formula: Q=CVQ = C V.
The charge stored by a capacitor is directly proportional to the potential difference across its terminals.
2
Perform the multiplication to determine the charge magnitude in microcoulombs.
Q=5.0×20.0=100.0 μCQ = 5.0 \times 20.0 = 100.0\text{ }\mu\text{C}.
Multiplying capacitance in microfarads by potential difference in volts yields charge directly in microcoulombs.

Key Concept

Fundamental relationship between capacitance, charge, and potential difference (Q=CVQ = C V)
Estimated Time:45s
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