Exams › JEE Main › Physics › Electric Charges and Fields
259 questions with worked solutions.
Q1. What is the SI unit of the permittivity of free space, ε₀?
Answer: coulomb²/newton-metre²
Coulomb's law F = q^2/(4*pi*eps0*r^2) gives eps0 = q^2/(F r^2). The units are coulomb^2/(newton x metre^2) = C^2 N^-1 m^-2, i.e. coulomb^2/newton-metre^2.
Q2. What is the SI unit used for electric flux?
Answer: volt metre
Electric flux = E . A. Since electric field has units V/m and area m^2, flux has units (V/m)(m^2) = V m (volt metre), equivalently N m^2 C^-1. The correct unit is volt metre.
Answer: 20 V m⁻¹
W = q*E*d*cos(theta): 10 = 0.5*E*2*cos60 = 0.5*E. So E = 20 V/m.
Answer: π/3 + tan⁻¹(√3/2)
At polar angle theta the dipole field tilts from the radius vector by beta with tan(beta) = (1/2)tan(theta) = (1/2)tan(60) = sqrt(3)/2. The field's angle with the x-axis is theta + beta = pi/3 + arctan(sqrt(3)/2).
Answer: λ/(2π ε₀ a)
The electric field at the center of a uniformly charged semicircular wire can be derived by integrating the contributions from each infinitesimal charge element along the semicircle. Due to symmetry, the horizontal components of the electric field cancel out, while the vertical components add up, resulting in a total electric field magnitude of λ/(2π ε₀ a).
Answer: p and r⁻³
The electric field due to an electric dipole at a point far away (where r is much greater than the dipole size) decreases with the cube of the distance (r⁻³) and is directly proportional to the dipole moment (p), which is why the correct option is p and r⁻³.
Answer: 2
Q_enc = integral of k r^a *4 pi r^2 dr gives E(r) = k r^(a+1)/(eps0 (a+3)), so E ~ r^(a+1). E(R/2)/E(R) = (1/2)^(a+1) = 1/8 = (1/2)^3, so a+1=3, a=2.
Answer: an excess of 4πr³(ρ−ρ0)g / 3Ee electrons
For equilibrium the electric force balances net gravity minus buoyancy: |q|E = (4/3)pi r^3 (rho0 - rho) g. Since rho0 > rho the charge must be negative, so the drop has an EXCESS of n = 4 pi r^3 (rho0-rho) g /(3 E e) electrons.
Answer: 8 V-m
The electric flux through a surface is calculated by taking the dot product of the electric field vector and the area vector. In this case, the dot product of E = 4î V/m and A = (2î + 3ĵ) m² results in 8 V-m, as only the î components contribute to the flux.
Answer: F/8
When sphere C, initially neutral, comes into contact with sphere A, it acquires a charge of +2q, and when it contacts sphere B, it acquires a charge of -2q. After these interactions, sphere A has a charge of +2q and sphere B has a charge of -2q, resulting in a new electrostatic force that is one-fourth of the original force F, leading to a final interaction force of F/8.
Answer: (1/4πϵ0) · 6p1p2/x⁴
The correct option is based on the derived formula for the force between two aligned electric dipoles, which shows that the force is proportional to the product of their dipole moments and inversely proportional to the fourth power of the distance between them, resulting in the factor of 6 in the numerator.
Q12. Identify the statement that is incorrect.
Answer: Charged particles cannot be created or annihilated.
The incorrect statement is 'Charged particles cannot be created or annihilated' - they can be (e.g., pair production/annihilation) provided net charge is conserved. The other three statements are all true.
Answer: √(4πϵ0 Fd²/e²)
The correct option relates the repulsive force between two positive ions to the number of electrons missing from each ion by using Coulomb's law. The formula shows that the force is proportional to the product of the charges (which are related to the number of missing electrons) and inversely proportional to the square of the distance between them, allowing us to derive the number of electrons in terms of the given variables.
Q14. Choose the incorrect statement about a conductor in electrostatic equilibrium.
Answer: At the surface of a charged conductor, the electrostatic field must be tangent to the surface at every point.
At the surface of a charged conductor the electrostatic field is perpendicular (normal) to the surface, not tangent to it. That statement is the incorrect one; the others are all true.
Answer: -Q/4
For the system to be in equilibrium, the net force acting on the charge q must be zero. The attractive forces from the two identical charges Q must balance the repulsive force from q, which occurs when q is negative and equal to -Q/4, allowing the forces to counteract each other.
Answer: (ϕ₂ − ϕ₁)/ε₀
According to Gauss's law, the net electric flux through a closed surface is directly proportional to the net charge enclosed within that surface. The net charge is calculated by subtracting the total flux entering the surface from the total flux leaving it, which is represented by (ϕ₂ − ϕ₁)/ε₀.
Answer: 2L
The zero-field point is outside the smaller (-2q) charge: 8q/x^2 = 2q/(x-L)^2 -> 2(x-L) = x -> x = 2L.
Answer: Both a torque and a translational force
In a non-uniform field the two charges of the dipole feel unequal forces, giving a net translational force; since the dipole is at 30 deg to the field it also feels a torque p x E. So it experiences both a torque and a translational force.
Answer: −2√2
For charge Q at a corner: the two q charges at the adjacent corners (distance L) give a resultant sqrt(2)*kQq/L^2 along the diagonal, and the opposite Q (distance L*sqrt(2)) gives kQ^2/(2L^2). Setting the net to zero: sqrt(2)*q + Q/2 = 0 -> Q/q = -2*sqrt(2).
Answer: Qr1²/(4π ε₀ R⁴)
Enclosed charge q(r1) = integral of (Q/pi R^4) r * 4 pi r^2 dr from 0 to r1 = Q r1^4 / R^4. Then E = q/(4 pi e0 r1^2) = Q r1^2 / (4 pi e0 R^4).
Answer: −6aϵ0
phi = a r^2 + b -> E = -dphi/dr = -2 a r. Using Gauss in spherical form, rho = e0*(1/r^2) d/dr(r^2 E) = e0*(1/r^2)(-6 a r^2) = -6 a e0. The charge density is -6 a e0.
Answer: y
The net force acting on the particle is due to the electric fields created by the two charges, which are symmetric about the y-axis. When the particle is displaced slightly along the y-axis, the forces from the two charges will create a restoring force that is proportional to the displacement y, indicating that the force acts in the direction of the displacement.
Answer: −Q/4
On the +Q at x=0: the +Q at x=d repels it, while q at x=d/2 must pull it back. Balancing kQ^2/d^2 = k Q|q|/(d/2)^2 = 4kQ|q|/d^2 gives |q| = Q/4, and q must be negative, so q = -Q/4.
Answer: R/√2
The axial field of a ring is E = kQx/(x^2+R^2)^(3/2). Setting dE/dx = 0 gives x^2 = R^2/2, so the field peaks at h = R/sqrt(2).
Answer: (10/9) volt/μ m and in the +ve x direction
V = 20/(x^2-4) -> dV/dx = -40x/(x^2-4)^2. At x=4: dV/dx = -160/144 = -10/9. So E = -dV/dx = +10/9 V/um, directed along +x.
Answer: Statement 1 is incorrect and Statement 2 is correct.
Statement 1 is incorrect because the change in potential energy when moving a charge from the center to the surface of the sphere does not equal qρ/(3ε0). However, Statement 2 is correct as it accurately describes the electric field inside the sphere, which is derived from the uniform charge distribution.
Answer: -80 J
The potential difference between two points in an electric field can be calculated using the formula V_A - V_O = - ∫_(O)^(A) E · dr. Here, integrating the electric field ext{E} = 30x² î from 0 to 2 meters results in a potential difference of -80 J, indicating that the potential at point A is lower than at point O.
Answer: 3F/8
Initially A = B = q, F = kq^2/d^2. C (0) touches A -> both q/2. Then C (q/2) touches B (q) -> each (q + q/2)/2 = 3q/4. New force = k(q/2)(3q/4)/d^2 = (3/8)kq^2/d^2 = 3F/8.
Answer: ρ₀R³/(12ε₀r²)
The correct option is derived from applying Gauss's law to the charge distribution of the solid ball. The charge density decreases linearly with radius, leading to a total charge that can be calculated and results in the electric field outside the ball being proportional to the total charge divided by the square of the distance from the center, yielding the specific form of the electric field as ρ₀R³/(12ε₀r²).
Answer: 5q
The magnetic force is always perpendicular to velocity and does no work, so only the electric force contributes: W = qE.d = q(2i+3j).(i+j) = q(2+3) = 5q.
Answer: R/√(2)
On the axis E ∝ x/(x^2 + R^2)^(3/2). Setting dE/dx = 0 gives x^2 = R^2/2, so the field is maximum at h = R/sqrt(2).
Answer: 180 V
E = 20x+10. V1 - V2 = -integral_{-5}^{1}(20x+10)dx = -[10x^2+10x]_{-5}^{1} = -(20 - 200) = 180 V.
Answer: E ∝ 1/D⁴
Total charge = 0 and dipole moment Sum(q*y) = 0, but the quadrupole moment Sum(q*y^2) = -6qd^2 is nonzero. A quadrupole field falls off as 1/D^4, so E ~ 1/D^4.
Answer: V = 0, E = 0
All 10 charges are equidistant R from the centre, so V = (k/R)(5(+q)+5(-q)) = 0. For E, summing the field vectors: the cosine/sine sums over the five +q positions (0,72,144,216,288 deg) and over the five -q positions (36,108,180,252,324 deg) each vanish (sum of 5 equally-spaced unit vectors = 0), so E_x = E_y = 0. Hence V = 0 and E = 0.
Answer: (3) (p)/(a)√((1)/(2πε₀ m a))
For collinear dipoles U = (1/4*pi*e0)*(2p^2/a^3). All of this converts to KE = m v^2 (both masses), giving v^2 = p^2/(2*pi*e0*m*a^3), so v = (p/a)*sqrt(1/(2*pi*e0*m*a)).
Answer: Only when the Gaussian surface is an equipotential surface and |E| is constant on the surface.
The simple form |E| = q_enc/(eps0|A|) requires that E be perpendicular to the surface (so the surface is equipotential) and that |E| be constant over it, so that the flux integral reduces to |E||A|. Both conditions must hold.
Answer: 0.424 nC m⁻²
The surface charge density at the intersection of the specified plane and the x-axis can be calculated using the formula that relates line charge density to surface charge density, taking into account the geometry of the charge distribution. Given the uniform line charge of 8 nC/m, the resulting surface charge density at the specified point is 0.424 nC/m².
Answer: 640
Flux = Ex * A = (2/5)(4.0x10^3)(0.4) = 1600 x 0.4 = 640 Nm^2/C.
Answer: 1.73 × 10¹⁰
m = (4/3)pi(2e-3)^3(3000) ~ 1.005e-4 kg; q = mg/E = (1.005e-4 x 9.81)/(3.55e5) ~ 2.78e-9 C; n = q/e ~ 2.78e-9/1.6e-19 ~ 1.73x10^10 electrons.
Answer: Q = 2q
To achieve maximum electrostatic repulsion between the two charges, the force between them, which is proportional to the product of the charges, should be maximized. The optimal division occurs when one charge is twice the other, leading to the relationship Q = 2q, which maximizes the product Q(Q - q) at a fixed total charge.
Answer: 4.44 μC
Line-charge field E = lambda/(2*pi*eps0*r) = 2k*lambda/r. Net force on dipole = q*2k*lambda*(1/r1 - 1/r2) with r1=0.010 m, r2=0.012 m: 2k*lambda = 2*9e9*3e-6 = 5.4e4, and (1/0.010 - 1/0.012) = 16.67 /m, so F = q*5.4e4*16.67 = q*9.0e5. Setting F = 4 N gives q = 4/9.0e5 = 4.44 microC.
Answer: (q²/(2πϵ0md³))^(1/2)
The correct option represents the angular frequency of simple harmonic motion for the proton, derived from the net force acting on it due to the two fixed electrons. The force is proportional to the displacement and inversely proportional to the cube of the distance, leading to the specific form of the frequency given by the equation.
Answer: 3
The electric flux through a surface is given by the product of the electric field and the area of the surface projected in the direction of the field. For the rectangular surface parallel to the y-z plane, the area is 0.2 m² and the electric field has a component of rac{4}{5} N/C in the j direction, resulting in a flux of 0.2 * rac{4}{5} = 0.16 N·m²/C. For the surface parallel to the x-z plane, the area is 0.3 m² and the electric field has a component of rac{3}{5} N/C in the i direction, resulting in a flux of 0.3 * rac{3}{5} = 0.18 N·m²/C. The ratio of these two fluxes is 0.16:0.18, which simplifies to 3:5, thus a = 3.
Answer: Statement I is true but Statement II is false
Statement I is correct because the electric field due to an electric dipole can exist within the sphere, but the net electric flux through a closed surface surrounding it is zero due to symmetry. Statement II is incorrect because, for a solid metallic sphere, the electric field inside is zero, and thus the electric flux through a closed surface inside the sphere must also be zero.
Answer: E = σ/(2ε0) (1 - Z/(Z² + R²)^(1/2))
The correct option accurately describes the electric field intensity along the z-axis due to a uniformly charged disc by incorporating the effects of both the surface charge density and the geometric relationship between the distance from the disc and its radius, leading to the correct expression for the electric field.
Answer: x = ((q² l)/(2πε₀ mg))^(1/3)
For small theta, separation x = 2*l*sin(theta) ~ 2*l*theta, and tan(theta) ~ x/(2l) equals the Coulomb-to-weight ratio k*q^2/(x^2*m*g). Setting x/(2l) = q^2/(4*pi*e0*x^2*m*g) gives x^3 = q^2*l/(2*pi*e0*m*g), so x = (q^2*l/(2*pi*e0*m*g))^(1/3).
Answer: At 5 cm from -5 μC on the right side of system
The third charged particle must be placed where the electric forces from both charges balance each other. At 5 cm from the -5 μC charge on the right side, the attractive force from the -5 μC charge and the repulsive force from the 20 μC charge will equalize, resulting in no net force on the third particle.
Q48. Which of the following physical quantities have the same dimensions ?
Answer: Electric displacement (D̄) and surface charge density
Electric displacement and surface charge density both represent the distribution of electric charge per unit area, thus they share the same dimensional formula, which is essential for understanding their relationship in electromagnetism.
Answer: 3.0 m
The electric field at point O, which is equidistant from both charges, is the result of the superposition of the fields created by each charge. Given the magnitudes of the charges and the calculated electric field strength, the distance 'd' can be derived using the formula for the electric field due to point charges, confirming that the correct distance is 3.0 m.
Answer: 3F/4
C (uncharged) touching A gives each q/2; C then touching B gives both 3q/4. At the midpoint (r/2 from each), force from B = k(3q/4)(3q/4)/(r/2)^2 = (9/4)F and from A = (3/2)F act oppositely, so net force on C = (9/4 - 3/2)F = 3F/4, option (3F/4).