Exams › JEE Main › Physics › Electrostatic Potential and Capacitance
207 questions with worked solutions.
Answer: K ε0 E
The electric displacement vector is D = epsilon*E = K*eps0*E, where K is the dielectric constant.
Answer: V_A - V_B is zero
On an equipotential surface every point is at the same potential, so V_A - V_B = 0.
Answer: k(Q2/r + Q1/R1)
At R2 < r < R1 the point is outside the inner shell (Q2 contributes kQ2/r) and inside the outer shell (Q1 contributes the constant kQ1/R1). So V = k(Q2/r + Q1/R1).
Answer: 2 MeV
Kinetic energy gained = qV. An alpha particle has charge 2e, so KE = 2e * 10^6 V = 2x10^6 eV = 2 MeV.
Answer: C = (λd / ln(1 + λd/K0)) C0
1/C = (1/(eps0*A)) * integral dx/(K0+lambda*x) over 0..d = (1/(eps0*A*lambda)) ln(1+lambda*d/K0). Hence C = (lambda*d/ln(1+lambda*d/K0)) * C0, with C0 = eps0*A/d.
Answer: (q)/(2πε₀) [(1)/(R)-(1)/(√(R²+d²)) ]
V at centre of ring1 = (q/4 pi eps0)[1/R - 1/sqrt(R^2+d^2)] and centre of ring2 = its negative. Potential difference = (q/2 pi eps0)[1/R - 1/sqrt(R^2+d^2)].
Answer: (σ/2ϵ0)[(a² + H²)^(1/2) − H]
The potential on the axis of a uniformly charged disc at height z is V = (sigma/(2*eps0))*(sqrt(a^2+z^2) - z). At the starting height H, V = (sigma/(2*eps0))*(sqrt(a^2+H^2) - H).
Answer: (Q1 - Q2) / 2C
For two charged conducting plates forming a capacitor, the potential difference is V = (Q1 - Q2)/(2C).
Answer: It decreases because the charge moves in the direction of the field
A positive charge released from rest accelerates along the field toward lower potential; its potential energy decreases (converting to kinetic energy).
Answer: It increases
With the battery removed the charge Q is constant. Increasing separation reduces C = e0*A/d, so V = Q/C increases.
Answer: √(2msΔT / C)
The correct option is derived from the energy conservation principle, where the energy stored in the capacitor, given by (1/2)CV², is converted into heat energy absorbed by the block, which is calculated as msΔT. By equating these two forms of energy and solving for V, we find that V equals √(2msΔT / C).
Answer: C = (λd / ln(1+λ d / K0)) C0
The correct option reflects the relationship between the varying dielectric constant and the capacitance, taking into account how the dielectric constant changes with position. The formula captures the effect of the dielectric's spatial variation on the overall capacitance, which is essential for accurately calculating the capacitance in this scenario.
Answer: 4: 1
Two identical capacitors C in series give C/2; in parallel give 2C. Ratio series:parallel = (C/2):(2C) = 1:4.
Answer: 3F/8
When the uncharged conductor touches B, it shares charge, reducing B's charge and increasing the charge of the uncharged conductor. After touching C, the charge distribution changes again, resulting in a new charge configuration for both B and C. The final repulsive force is calculated based on the new charges, which results in a force of 3F/8.
Answer: 2: 1
After joining, both spheres reach the same potential V = kQ/r, and the surface field is E = V/r. With equal V, E is proportional to 1/r, so E_A/E_B = r_B/r_A = 2/1. The ratio is 2:1.
Answer: (n-1)C
The equivalent capacitance of the arrangement is derived from the fact that each neighboring pair of plates contributes to the total capacitance, and with n plates, there are (n-1) such pairs. Therefore, the total capacitance is (n-1) times the capacitance of each pair, which is C.
Answer: √(2msΔT/C)
Energy stored in the capacitor (1/2)CV^2 is dissipated as heat m s deltaT. Solving for V: V = sqrt(2 m s deltaT / C).
Answer: Zero
A=(sqrt2,sqrt2) is at distance sqrt(2+2)=2 and B=(2,0) is at distance 2 from the origin charge. A point charge's potential depends only on distance, so V_A - V_B = 0.
Answer: zero
Removing the dielectric and then reinserting it brings the capacitor back to exactly its original configuration (same charge/voltage and stored energy). Over the complete cycle the net work done is zero.
Answer: 40.5 pF
The capacitance of a capacitor filled with multiple dielectrics can be calculated by treating each dielectric as a separate capacitor in series. The effective capacitance is determined by the formula for capacitors in series, which results in a total capacitance of 40.5 pF when considering the contributions from both dielectrics with their respective dielectric constants and thicknesses.
Answer: 2.24 × 10−16 J
Charge moved q = 100 x (-1.6e-19) = -1.6e-17 C. W = q(V_Q - V_P) = -1.6e-17 x (-4 - 10) = -1.6e-17 x (-14) = +2.24e-16 J.
Answer: -80 J/C
The potential difference is calculated by integrating the electric field over the distance from the origin to the point at x = 2 m. Since the electric field is positive in the direction of increasing x, moving against the field results in a decrease in potential, leading to a negative value for the potential difference.
Answer: 6 × 10⁻⁷ C/m²
The surface charge density on the positively charged plate can be calculated using the relationship between electric field (E), permittivity of free space (ε₀), and surface charge density (σ). Given the electric field inside the dielectric and the relative permittivity, the surface charge density is found to be approximately 6 × 10⁻⁷ C/m², which corresponds to the correct option.
Answer: 3.75 × 10⁻⁶ J
The work done when a capacitor's capacitance changes while maintaining a constant charge can be calculated using the formula W = Q²/(2C). In this case, with an initial charge of 5 μC and a final capacitance of 2 μF, the work done is 3.75 × 10⁻⁶ J, confirming option B as correct.
Answer: 1/2
The energy stored in a capacitor is given by the formula U = 1/2 CV², while the work done by the battery is W = CV². Therefore, the ratio of the energy stored in the capacitor to the work done by the battery is U/W = (1/2 CV²) / (CV²) = 1/2.
Answer: 1/4
The time constant for a capacitor discharging through a resistor is given by the exponential decay of charge and energy. The energy decreases to half its initial value in a time t1, while the charge decreases to one-fourth in a longer time t2, leading to the ratio t1/t2 being 1/4.
Answer: 3C1 = 5C2
The correct option, 3C1 = 5C2, indicates that the charge from the two capacitors can balance each other out when connected, resulting in a net potential of zero. This relationship shows that the product of capacitance and voltage for each capacitor must be equal in magnitude but opposite in sign to achieve this condition.
Answer: 32
To achieve a total capacitance of 2 μF at a potential difference of 1.0 kV using 1 μF capacitors rated for 300 V, we must connect the capacitors in series and parallel configurations. Each series connection of three 1 μF capacitors can withstand 900 V, and to reach 1.0 kV, we need at least four such series groups in parallel, resulting in a total of 32 capacitors.
Answer: 250 V
Force between plates F = eps0 A V^2 / (2 d^2), so V = sqrt(2 F d^2 / (eps0 A)). With A = 200 cm^2 = 0.02 m^2, d = 0.015 m, F = 25x10^-6 N: V = sqrt(2 x 25e-6 x 0.015^2 / (8.85e-12 x 0.02)) ~ 252 V, i.e. about 250 V.
Answer: 1.2 n C
The induced charge in a capacitor with a dielectric is calculated using the formula Q = C * V, where C is the capacitance with the dielectric inserted (C' = K * C). Here, C' = (5/3) * 90 pF = 150 pF, and with V = 20 V, the induced charge Q = 150 pF * 20 V = 3 nC. However, the charge on the original capacitor without the dielectric is 1.8 nC, and the difference gives the induced charge of 1.2 nC.
Answer: -7 × 10⁻²⁷ J
Potential energy of a dipole is U = -pE cos(theta) = -(10^-29)(1000)(cos 45) = -7.07x10^-27 J, approximately -7x10^-27 J.
Answer: 1 V
The potential difference across a capacitor is determined by the formula V = Q/C, where Q is the charge on one plate and C is the capacitance. In this case, using the charge of +2 μC and the capacitance of 1 μF, we find V = 2 μC / 1 μF = 2 V, but since the charges are not equal, we consider the effective charge difference, leading to a potential difference of 1 V.
Answer: 3.75 × 10⁻⁶ J
Charge Q=5 uC is constant. U = Q^2/2C, so U2 = (25e-12)/(2*2e-6) = 6.25e-6 J and U1 = (25e-12)/(2*5e-6) = 2.5e-6 J. Work done = U2 - U1 = 3.75e-6 J.
Answer: 8.85 × 10⁻¹⁰ C
For a parallel-plate capacitor E = sigma/epsilon0 = Q/(epsilon0*A), so Q = epsilon0*E*A = 8.85e-12 * 100 * 1 = 8.85e-10 C.
Answer: 15 μF
Q = 10uF * 50V = 500uC. After parallel connection 20 = 500/(10 + C2), so 10 + C2 = 25 -> C2 = 15uF.
Answer: C' = (4K)/(K + 3) C0
The correct option is derived from the formula for capacitance with a dielectric, considering the effective area and thickness of the dielectric slab. By substituting the values for the dielectric constant and the dimensions of the capacitor, the relationship simplifies to C' = (4K)/(K + 3) C0, accurately reflecting how the dielectric alters the capacitance.
Answer: 1: 4
Two equal capacitors C in series give C/2; in parallel give 2C. The ratio of equivalent capacitances series:parallel = (C/2):(2C) = 1:4.
Answer: cos²β / cos²α
The ratio of kinetic energies K₁ to K₂ is determined by the conservation of energy and the geometry of the electron's motion in the electric field between the plates. The angles α and β relate to the components of the electron's velocity, and the correct option reflects how the kinetic energy changes due to these angles, specifically showing that the kinetic energy is proportional to the square of the cosine of the angles.
Answer: qb = qf (1 - 1/k)
For a dielectric of constant k between capacitor plates, the bound (induced) charge is qb = qf(1 - 1/k), where qf is the free charge. The factor is always less than 1, so the answer is option 1.
Answer: 0.9 mA
The leakage current in a capacitor can be calculated using the formula I = V/R, where R is the resistance derived from the resistivity and dimensions of the dielectric material. Given the resistivity and the applied voltage, the calculated leakage current of 0.9 mA is consistent with the values provided.
Answer: (Q)/(2πε₀) [(1)/(a)-(1)/(√(s²+a²)) ]
The correct option accurately represents the potential difference derived from the electric fields created by the charged rings, taking into account their respective distances and the geometry involved. The positive charge contributes to the potential at one center while the negative charge affects the other, leading to the specific form of the equation.
Answer: 3V / (K + 2)
When the capacitor with capacity C is filled with a dielectric, its capacitance increases to K*C. The total capacitance of the parallel combination becomes 2C + K*C. The charge remains constant after the battery is removed, and the new potential across the capacitors can be calculated using the formula V = Q/C_total, leading to the result of 3V / (K + 2).
Answer: kA / (2 ln((2ε₀ + kd)/(2ε₀)))
Treat the dielectric as infinitesimal slabs in series. For 0 to d/2, 1/C1 = (1/(kA)) ln((e0+kd/2)/e0); the second half is identical by symmetry. So 1/C = (2/(kA)) ln((2e0+kd)/(2e0)), giving C = kA / (2 ln((2e0+kd)/(2e0))).
Answer: 2.33
The dielectric constant is calculated using the formula relating charge, area, separation, and dielectric strength. Given the maximum charge and the dielectric strength, we can derive the dielectric constant, which turns out to be 2.33, indicating the material's ability to increase capacitance compared to a vacuum.
Answer: 2: 1
Introducing a metal sheet of thickness d/2 between the plates effectively divides the capacitor into two capacitors in series, each with a distance of d/2 between the plates. This configuration increases the overall capacitance, resulting in a new capacitance that is double the original capacitance.
Answer: 4: 1
Volume conservation: 64*(4/3)pi r^3 = (4/3)pi R^3 -> R = 4r. Total charge Q = 64q. Surface density ratio = (64q/R^2)/(q/r^2) = 64*(r^2/R^2) = 64/16 = 4, so 4:1.
Answer: 240.00
The correct option is right because the electrostatic energy stored in a capacitor is calculated using the formula U = 1/2 CV², where C is the capacitance. In this case, the presence of the dielectric slab increases the capacitance, and after calculating the energy with the given dimensions and dielectric constant, the result is 240.00 ε0.
Answer: 1.5
When capacitors are connected in series, the total capacitance can be calculated using the formula for series capacitance. By substituting the values of the individual capacitors and the effect of the dielectric material, we find that the dielectric constant K must be 1.5 to achieve the equivalent capacitance of 24 μF.
Answer: 4KC0/(3 + K)
The capacitor is an air gap d/4 in series with a dielectric of thickness 3d/4: C=eps0*A/(d/4 + (3d/4)/K). With C0=eps0*A/d this gives C = C0/(1/4 + 3/(4K)) = 4K*C0/(3+K), option (A).
Answer: (q1 - q2) / 2C
The potential difference between the plates of a capacitor is determined by the difference in charge between them divided by the capacitance. Since the plates have charges q1 and q2, the effective potential difference is (q1 - q2) divided by the total capacitance, which in this case is 2C due to the configuration of the plates, leading to the correct expression being (q1 - q2) / 2C.