Exams › JEE Main › Physics › Moving Charges and Magnetism
194 questions with worked solutions.
Answer: 1.5 × 10⁻² N-m
tau = N*I*A*B*sin(30) = 2000 * 2.0 * 1.5e-4 * 5e-2 * 0.5 = 1.5e-2 N-m.
Answer: B = 2πmν / e and K = 2mπ²ν²R²
Cyclotron resonance: nu = eB/(2 pi m) so B = 2 pi m nu/e. v_max = 2 pi nu R, so K = (1/2)m(2 pi nu R)^2 = 2 m pi^2 nu^2 R^2.
Answer: 1
The magnetic field inside a long, straight conductor increases linearly with distance from the center, while outside the conductor, it decreases with the distance from the axis. At a distance a/2, the magnetic field is proportional to the distance from the center, while at 2a, it behaves inversely with distance, leading to a ratio of 1.
Answer: 1.25 m
I = q*f = 2e-6 * 6.25e12 = 1.25e7 A. From B = mu0*I/(2r), r = mu0*I/(2B) = (4*pi*1e-7 * 1.25e7)/(2*6.28) = 1.25 m.
Answer: 40 m/s
For undeflected motion the electric and magnetic forces balance: qE = qvB, so v = E/B = 20/0.5 = 40 m/s.
Answer: sin−1[ Bd (q/2mV)1/2 ]
From qV=(1/2)mv^2, v=sqrt(2qV/m); radius r=mv/(qB). Deflection angle theta has sin(theta)=d/r = Bd*(q/(2mV))^(1/2), so theta = sin^-1[Bd(q/2mV)^(1/2)].
Answer: q and m
Magnetic moment = (1/2)*q*omega*r^2 and angular momentum = m*omega*r^2, so their ratio = q/(2m), which depends only on q and m.
Answer: It is proportional to 1/R²
From qV = (1/2)mv^2 and R = mv/(qB): q/m = 2V/(R^2 B^2), so q/m is proportional to 1/R^2.
Answer: n²B
When the wire is wound into a coil with n turns, the magnetic field at the center increases because each turn contributes to the total magnetic field. The magnetic field strength is proportional to the number of turns squared, resulting in a field strength of n²B at the center.
Answer: its momentum varies, while its kinetic energy remains unchanged
The magnetic force is perpendicular to velocity, so it does no work: kinetic energy (and speed) stay constant. Momentum is a vector whose direction continuously changes, so momentum varies.
Answer: a straight path
From rest, only E acts initially, accelerating the particle along B. Since the velocity stays parallel to B, the magnetic force qv x B is always zero, so the path is a straight line along the field.
Answer: 2(τ/√3Bl)^(1/2)
With B in the coil's plane, torque tau = i*A*B = i*(sqrt3/4)*l^2*B. Solving, l = 2*sqrt(tau/(sqrt3 * B * i)), which is index 1.
Q13. A magnetic needle is placed in a magnetic field that is not uniform. What will it experience?
Answer: Both force and torque
In a non-uniform magnetic field, the magnetic needle experiences a gradient in the magnetic field strength, which results in both a force acting on it and a torque that tends to align it with the field. The force arises from the variation in magnetic field strength across the needle, while the torque is due to the interaction of the needle's magnetic moment with the field.
Q14. A dead-beat galvanometer shows a pointer that quickly comes to rest at a fixed reading because
Answer: eddy currents are set up in the metallic frame supporting the coil.
A dead-beat galvanometer has its coil wound on a metallic (conducting) frame; the induced eddy currents oppose the motion, quickly damping oscillations so the pointer settles fast.
Q15. When an electric current flows through a spring, what happens to it?
Answer: It contracts
When an electric current flows through a spring, it generates heat due to resistance, causing the material to expand initially but then contract as it cools down, resulting in an overall contraction.
Answer: 1
The magnetic field at the center of a circular loop is directly proportional to the current and inversely proportional to the radius. For loop A, the field is proportional to I/R, and for loop B, it is proportional to (2I)/(2R). Simplifying both expressions shows that they are equal, resulting in a ratio of 1.
Answer: Their trajectories will have the same curvature, apart from the direction of rotation.
Both the electron and the proton experience the same magnetic force due to their equal momentum and perpendicular entry into the magnetic field, resulting in circular paths. However, the electron, being lighter, will have a faster angular velocity, leading to the same curvature but opposite rotation direction.
Answer: speed
The time period of a charged particle moving in a magnetic field is determined by the radius of the circular path and the magnetic field strength, and it remains constant regardless of the particle's speed. This is because the magnetic force provides the necessary centripetal force, leading to a fixed frequency of rotation.
Answer: zero
The work done by a magnetic field on a charged particle is always zero because the magnetic force acts perpendicular to the velocity of the particle, resulting in no displacement in the direction of the force.
Answer: n²B
Fixed wire length L = 2*pi*R. With n turns each radius r = R/n. B' = n*mu0*I/(2r) = n*mu0*I/(2R/n) = n^2 * mu0*I/(2R) = n^2 B.
Answer: 250 μT
B_centre = B_axis*(R^2+x^2)^(3/2)/R^3 = 54*(3^2+4^2)^(3/2)/3^3 = 54*125/27 = 250 microT.
Answer: -2F/3
F = mu0*I1*I2/(2*pi*d). Doubling one current and tripling the separation scales the magnitude by 2/3, and reversing that current flips attraction to repulsion (sign change). New force = -2F/3.
Answer: 5 × 10⁻⁵
The magnetic induction at the center of two perpendicular coils can be calculated using the formula for the magnetic field due to a circular coil, which is proportional to the current and inversely proportional to the radius. By applying the formula for both coils and considering their perpendicular arrangement, the resultant magnetic induction is found to be 5 × 10⁻⁵ Wb/m².
Answer: 2πm/qB
The period of revolution for a charged particle in a magnetic field is derived from the balance of the magnetic force and the centripetal force, leading to the formula T = 2πm/(qB), where T is the period, m is the mass, q is the charge, and B is the magnetic field strength.
Answer: attract one another with a force of μ0i²/(2πd)
Two long parallel wires carrying current in the same direction attract each other, with force per unit length F/L = mu0*i^2/(2*pi*d).
Answer: straight path
The charge starts at rest, so qE accelerates it along E, which is parallel to B. Its velocity stays parallel to B, making qv x B = 0 at all times. It therefore moves in a straight line.
Answer: 1.05 × 10⁻² Weber/m²
B = mu0*n*i, so B2 = B1*(n2/n1)*(i2/i1) = 6.28e-2*(100/200)*(1/3) = 1.05e-2 Wb/m^2.
Answer: 1
At a/2 (inside): B = mu0*i*(a/2)/(2*pi*a^2) = mu0*i/(4*pi*a). At 2a (outside): B = mu0*i/(2*pi*2a) = mu0*i/(4*pi*a). The two are equal, so the ratio is 1.
Q29. A current I flows along the length of an infinitely long, straight, thin walled pipe. Then
Answer: the magnetic field at any point inside the pipe is zero
According to Ampère's law and the properties of magnetic fields generated by current-carrying conductors, the magnetic field inside a hollow conductor is zero due to the symmetry of the current distribution, which results in the cancellation of the magnetic field lines.
Answer: v = E × B / B²
The correct option is derived from the condition that the net force acting on the charged particle must be zero for it to maintain its velocity. In a uniform electric field E and magnetic field B, the electric force qE and the magnetic force q(v × B) must balance each other, leading to the relationship v = E × B / B².
Q31. A charged particle moves through a magnetic field perpendicular to its direction. Then
Answer: the momentum changes but the kinetic energy is constant
When a charged particle moves through a magnetic field perpendicular to its velocity, the magnetic force acts as a centripetal force, changing the direction of the particle's momentum without altering its speed. Since the speed remains constant, the kinetic energy, which depends on speed, also remains constant.
Answer: (d) μ0I / π2R
The magnetic induction along the axis of a semi-circular wire can be derived using the Biot-Savart law, which shows that the contribution to the magnetic field from each segment of the wire adds up to yield the result of μ0I / π2R. This reflects the unique geometry of the semi-circular shape, which influences the field strength along the axis.
Answer: 11 q
v x B = (3,4,1) x (1,1,-3) = (-13,10,-1). E + v x B = (-10,11,1). The force is q times this, so the y-component is 11q.
Answer: (b) r_α = rₚ < r_d
For equal KE, r = sqrt(2mE)/(qB) ~ sqrt(m)/q. Proton: sqrt(1)/1=1; deuteron: sqrt(2)/1=1.41; alpha: sqrt(4)/2=1. Hence r_alpha = r_p < r_d (option b).
Answer: F₁ = F₂ = 0
The magnetic fields inside coaxial solenoids do not exert forces on each other when they carry the same current in the same direction, resulting in zero net force on both solenoids.
Answer: π²/(8√2)
The magnetic field at the center of a circular loop is given by the formula B = (μ₀I)/(2R), while for a square loop, it can be derived to be B = (μ₀I)/(4a) multiplied by a correction factor due to the geometry. Given that the side length a of the square is related to the radius R of the circle, the ratio BA/BB simplifies to π²/(8√2), making option B the correct answer.
Answer: rₑ < rₚ = r_α
The radius of the circular orbit in a magnetic field is directly proportional to the momentum of the particle and inversely proportional to its charge. Since the electron has a much smaller mass and charge compared to the proton and alpha particle, it will have a smaller radius for the same kinetic energy, leading to the relation rₑ < rₚ = r_α, as both the proton and alpha particle have the same charge-to-mass ratio.
Answer: √2
The magnetic dipole moment of a circular loop is directly proportional to the current and the area of the loop. When the dipole moment is doubled while keeping the current constant, the area must also double, leading to an increase in the magnetic field strength at the center of the loop by a factor of √2, resulting in the ratio B1/B2 being √2.
Answer: 0.27 Nm
m = N*i*A = 100*3*(0.05*0.025) = 0.375 A m^2. With coil in X-Z plane its normal is along Y (perpendicular to B along X). Tilting 45 deg about Z makes the angle between m and B equal 45 deg, so tau = m*B*sin45 = 0.375*1*0.707 = 0.27 Nm.
Answer: 4 × 10⁻⁵ Wb/m²
For an equilateral triangle, perpendicular distance from centre to a side d = a/(2*sqrt(3)). Field from one side = (mu0*I/4pi/d)*2*sin60. With a=4.5e-2 m, I=1 A, each side gives ~1.33e-5 T; three sides total ~4e-5 Wb/m^2.
Answer: 2.0 × 10⁻²⁴ kg
Straight-line motion needs qE=qvB so v=E/B=100/0.5=200 m/s. From r=mv/(qB), m=qBr/v=(1.6e-19*0.5*0.005)/200 = 2.0e-24 kg.
Answer: rₑ < rₚ = r_he
For equal energy, r = sqrt(2mE)/(qB) so r is proportional to sqrt(m)/q. For He: sqrt(4m_p)/2 = sqrt(m_p)/1 = same as proton, so r_p = r_he. The electron's tiny mass makes r_e the smallest, giving r_e < r_p = r_he.
Answer: 4m/π
Square side a gives m = I a^2 with perimeter 4a. Same wire forms a circle: 2*pi*r = 4a => r = 2a/pi, area = pi r^2 = 4a^2/pi. So m_circle = I*(4a^2/pi) = 4m/pi.
Answer: 0.27 N m
The torque on a coil in a magnetic field is calculated using the formula τ = n * I * A * B * sin(θ), where n is the number of turns, I is the current, A is the area of the coil, B is the magnetic field strength, and θ is the angle between the magnetic field and the normal to the coil's plane. In this case, the area of the coil is 0.0125 m², the angle after tilting is 45°, and substituting these values gives the correct torque of 0.27 N m.
Answer: 10⁻²
The correct option is 10⁻² because the deflection angle of the coil is directly related to the magnetic field strength, the current, and the physical properties of the coil. Using the formula for torque in a galvanometer, we can derive that the magnetic field strength must be approximately 0.01 T to produce a 10° deflection at 1 mA.
Answer: 7.5 × 10⁻⁴ m
The correct option is right because the radius of the path of an electron in a magnetic field is determined by the balance between the centripetal force and the magnetic force acting on the electron. By calculating the velocity gained from the applied voltage and using the formula for the radius of circular motion in a magnetic field, the result yields a radius of 7.5 × 10⁻⁴ m.
Answer: 4 cm
T = 2*pi*(1.67e-27)/(1.69e-19*0.3) = 2.07e-7 s. Pitch = v*cos60*T = 4e5*0.5*2.07e-7 = 0.041 m ~ 4 cm.
Answer: (3) −30i + 32j − 9k
v x B = (-30, 32, -9)*10^-3. F = q(v x B) = 10^-6 * (-30,32,-9)*10^-3 = (-30,32,-9)*10^-9 N, so F = -30i + 32j - 9k.
Answer: 4.8 × 10⁻¹⁹ N
B_max = E_max/c = 30/(3e8) = 1e-7 T. v = 0.1c = 3e7 m/s. F = qvB = 1.6e-19 * 3e7 * 1e-7 = 4.8e-19 N.
Answer: (4) qdB0/m
The particle follows a circular arc whose maximum penetration toward the screen equals its radius r = mv/(qB0). It just fails to reach a screen at distance d when r = d, giving the critical speed v = qdB0/m.