Exams › JEE Main › Physics › System of Particles and Rotational Motion
298 questions with worked solutions.
Answer: -αv²/M
The correct option is right because the satellite's acceleration is derived from the change in momentum due to the mass being collected at a rate proportional to its velocity. As the satellite gathers mass, the force exerted by the collected dust results in a negative acceleration, which is accurately represented by the equation -αv²/M, where M is the mass of the satellite.
Answer: 7F/8
Total mass = m + m/3 = 4m/3, so a = F/(4m/3) = 3F/(4m). Mass behind the rope's midpoint = block + half the rope = m + m/6 = 7m/6. Tension there = (7m/6)*a = (7m/6)(3F/4m) = 7F/8.
Answer: mF/(m + M)
The whole system accelerates at a = F/(m+M). The only horizontal force on block m is the spring force, which must equal m*a = mF/(m+M).
Answer: (b) Mm/(M+2m) × ω² R²
The correct option reflects the change in the moment of inertia of the system when the two small masses are added to the ring, which affects the total kinetic energy. The decrease in kinetic energy is calculated by considering the initial and final moments of inertia and their corresponding angular velocities, leading to the expression given in option (b).
Answer: K²/(K² + R²)
With I = mK^2 and v = wR, KE_rot/KE_total = (1/2 I w^2)/((1/2 I w^2)+(1/2 m v^2)) = K^2/(K^2 + R^2).
Answer: 3/4
When a 90° arc is removed from the uniform circular ring, the remaining portion consists of three-quarters of the original mass and retains the same radius. The moment of inertia of the full ring is MR², and removing the arc reduces the moment of inertia proportionally, resulting in a new moment of inertia of (3/4)MR².
Answer: √(6g/l) sin(θ/2)
With I = ml^2/3 about the end and the centre of mass falling (l/2)(1-cos th) from the inverted position: (1/2)(ml^2/3)w^2 = mg(l/2)(1-cos th). Thus w^2 = (3g/l)(1-cos th) = (6g/l)sin^2(th/2), so w = sqrt(6g/l) sin(th/2).
Answer: (1/24) A l³ ρ ω²
For rotation about the perpendicular axis YY' through the rod's centre, I = (1/12) M l^2 with M = A l rho. KE = (1/2) I w^2 = (1/2)(1/12)(A l rho) l^2 w^2 = (1/24) A l^3 rho w^2.
Answer: 7.1 m
A solid sphere rolling without slipping has total KE = (7/10) m v^2 (translational + rotational). Setting (7/10) m v^2 = m g h gives h = 7 v^2/(10 g) = 7*100/98 ~ 7.14 m, i.e. about 7.1 m.
Q10. What type of motion is produced by a couple?
Answer: Only rotational motion
A couple consists of two equal and opposite forces, so the net force is zero (no translation) but the net torque is nonzero, producing only rotational motion.
Answer: 43 kgm²
The moment of inertia about the x-axis is calculated by summing the products of each mass and the square of its perpendicular distance from the x-axis. For the given masses and their coordinates, the distances are 0, 3, 2, and 2, leading to a total moment of inertia of 43 kgm².
Answer: constant in magnitude
For rolling without slipping with the centre moving at constant v0, any rim point has only centripetal acceleration toward the centre of magnitude omega^2 R = v0^2/R. This magnitude is constant, but the direction continuously points from the rim point to the centre and so rotates. Thus the acceleration is constant in magnitude only.
Answer: 2 s
KE = (1/2)I w^2 = 1500 gives w^2 = 2500, w = 50 rad/s. With alpha = 25, t = w/alpha = 50/25 = 2 s.
Answer: greater than 3 but less than 6
Torque = F*r = (20t-5t^2)*2; alpha = torque/I = (40t-10t^2)/10 = 4t - t^2. omega = 2t^2 - t^3/3, which returns to zero at t=6 s. theta = integral omega dt = 2t^3/3 - t^4/12 = 144 - 108 = 36 rad at t=6. Revolutions = 36/(2pi) = 5.7, i.e. greater than 3 but less than 6.
Answer: Her moment of inertia decreases
Bringing arms and legs inward reduces the distribution of mass about the spin axis, so the moment of inertia decreases. With angular momentum conserved, the angular velocity correspondingly increases.
Answer: 4πMR²/5T
For a uniform solid sphere, I = (2/5)MR^2 and omega = 2pi/T. Angular momentum L = I*omega = (2/5)MR^2*(2pi/T) = 4 pi M R^2/(5T).
Answer: ((8.02)⁴-(7.98)⁴)/(0.8)⁴
Tube J ~ (Ro^4 - Ri^4) = (8.02^4 - 7.98^4). Equal-volume solid rod: 2*pi*R*t = pi*r^2 -> r^2 = 2*8*0.04 = 0.64 -> r = 0.8, so J_rod ~ 0.8^4. Ratio = ((8.02)^4-(7.98)^4)/(0.8)^4.
Answer: The magnitude of the torque due to gravity about O is decreasing
The torque due to gravity about point O depends on the perpendicular distance from O to the line of action of the gravitational force. As the particle falls, this distance decreases, leading to a reduction in the magnitude of the torque.
Answer: (M/(M + 4m)) ω1
The final angular velocity is derived from the conservation of angular momentum, where the initial angular momentum of the disc must equal the final angular momentum after the spheres are added. Since the spheres are added at diametrically opposite points, their contribution to the moment of inertia effectively increases the total moment of inertia of the system, leading to a decrease in angular velocity.
Answer: v/2
The velocity of the center of mass is calculated using the formula v_cm = (m1*v1 + m2*v2) / (m1 + m2). Since the particles are identical, their masses are equal, and the center of mass velocity is the average of their velocities, which results in v/2.
Q21. Moment of inertia of a circular wire of mass M and radius R about its diameter is
Answer: MR²/2
The moment of inertia of a circular wire about its diameter is derived from the integral of mass distribution, which results in the formula MR²/2, indicating that the mass is evenly distributed along the circular path.
Answer: I_y = 64 Iₓ
The moment of inertia for a disc is proportional to its mass and the square of its radius. Disc Y, having a radius 4R and a thickness t/4, has a mass that scales with the volume, resulting in a factor of 16 increase due to the radius squared and an additional factor of 4 due to the thickness, leading to a total increase of 64 times the moment of inertia of disc X.
Answer: L/4
In uniform circular motion, angular momentum (L) is proportional to angular frequency (ω) and the moment of inertia (I). If the angular frequency is doubled (2ω) and the kinetic energy is halved, the relationship between kinetic energy and angular momentum shows that the new angular momentum is reduced to a quarter of the original, resulting in L/4.
Answer: no shift occurs
Splitting is due to internal forces; the only external force is gravity, which acts identically on the combined fragments. The centre of mass of B and C continues along the original trajectory of A, so there is no shift relative to it.
Answer: 1/2 Mr²
For a full disc I = (1/2)MR^2. A semicircular lamina is half the disc with half the mass, so the ratio I/M is unchanged: I = (1/2)Mr^2 about the perpendicular axis through the centre.
Answer: (m1/m2) d
To hold the centre of mass fixed the mass-weighted displacements must cancel: m1*d = m2*d2, so the second particle must move (in the opposite sense) by d2 = (m1/m2) d.
Answer: 3mℓ²
Place A(0,0),B(l,0),C(l,l),D(0,l). The line through A parallel to BD is x+y=0; distance of a point is |x+y|/sqrt2. Contributions: A 0, B m*l^2/2, D m*l^2/2, C m*(2l^2). Total = 3 m l^2.
Answer: ωm/(m + 2M)
The correct option is derived from the conservation of angular momentum. Initially, the hoop has angular momentum based on its mass and angular speed. When the two point masses are added, the total mass of the system increases, and to conserve angular momentum, the new angular speed must decrease, resulting in the formula ωm/(m + 2M).
Answer: 1/3
Mass scales with area: big disc (radius 2R) ~ 4m, removed disc (radius R) ~ m, with the small disc's center at distance R from the big center. COM = (4m.0 - m.R)/(4m - m) = -R/3, so the remaining lamina's COM is at R/3, i.e. alpha = 1/3.
Q30. The angular momentum of a particle moving under a central force remains unchanged because the
Answer: torque acting on it is zero
The angular momentum of a particle remains constant when the net torque acting on it is zero, which occurs in a central force scenario where the force is directed towards a fixed point, resulting in no rotational influence.
Answer: increases at first and then decreases
As the insect moves from the edge towards the center of the disc, it reduces the moment of inertia of the system, which causes the angular speed to increase due to conservation of angular momentum. However, as it reaches the opposite edge, the moment of inertia increases again, leading to a decrease in angular speed.
Answer: rω0/2
Angular momentum about the contact line is conserved: mr^2*w0 = Iw + mvr = mr^2(v/r) + mvr = 2mvr, giving v = r*w0/2.
Answer: Its direction changes, but its magnitude remains constant.
The angular momentum of the mass remains constant in magnitude because the speed and distance from the axis of rotation do not change, but its direction changes continuously as the mass moves in a circular path.
Answer: 3h/4
The center of mass of a solid cone is located at a distance of 3h/4 from the vertex along its axis, which accounts for the distribution of mass being denser towards the base due to the cone's shape.
Answer: 4MR²/(9√3π)
Largest inscribed cube has a = 2R/sqrt3. Cube mass = M*(a^3)/((4/3)pi R^3) = 2M/(sqrt3 pi). I about axis normal to a face = (1/6) m a^2 = (1/6)*(2M/(sqrt3 pi))*(4R^2/3) = 4MR^2/(9 sqrt3 pi).
Answer: 2k/I θ
The kinetic energy of the disc is given as kθ², and using the relationship between kinetic energy and angular motion, we can derive that the angular acceleration is proportional to the torque applied, which results in the expression 2k/I θ, indicating that the angular acceleration increases with the angle of rotation.
Answer: 14: 15: 20
Energy conservation gives h = (v^2/2g)(1 + k^2/R^2). For ring, solid cylinder and solid sphere, (1 + k^2/R^2) = 2 : 3/2 : 7/5 = 20 : 15 : 14, i.e. the heights are in the ratio 14 : 15 : 20.
Answer: √(7/48) l
By parallel axis, I = (1/12) m l^2 + m (l/4)^2 = m l^2 (1/12 + 1/16) = 7 m l^2 / 48. Radius of gyration k = sqrt(I/m) = sqrt(7/48) l.
Answer: H sin α + G cos α
The moment of a couple is determined by the perpendicular distance between the lines of action of the forces. When one force is rotated through an angle α, the new moment can be expressed as the sum of the original moment G adjusted by the cosine of α and the new moment H adjusted by the sine of α, leading to the correct expression H sin α + G cos α.
Answer: π/6
The torque is given by the formula τ = r × F × sin(θ), where τ is the torque, r is the distance from the origin, F is the force, and θ is the angle between the force and the position vector. Rearranging the formula and substituting the known values, we find that the angle θ that satisfies the equation for the given torque and force is π/6 radians.
Answer: 2k/I θ
KE = k*theta^2, so torque = d(KE)/d(theta) = 2k*theta = I*alpha. Hence angular acceleration alpha = 2k*theta/I.
Answer: rₙ ∝ √n, Eₙ ∝ n
Central force F = kr gives mv^2/r = kr so v ~ r. Quantization mvr = n*hbar with v ~ r gives r^2 ~ n, i.e. r_n ~ sqrt(n). Energy E = (1/2)mv^2 + (1/2)k r^2 ~ r^2 ~ n, so E_n ~ n. Hence r_n ~ sqrt(n), E_n ~ n.
Answer: 195
The torque is calculated using the cross product of the position vector from the point of rotation to the point of force application and the force vector. After computing the cross product and finding the magnitude, we determine that the value of x is 195.
Answer: 7ML²/18
With lambda = lambda0(1 + x/L), total mass M = integral_0^L lambda dx = 3*lambda0*L/2, so lambda0 = 2M/(3L). Moment of inertia about A: I = integral_0^L x^2*lambda dx = lambda0*(L^3/3 + L^3/4) = lambda0*7L^3/12 = 7ML^2/18.
Answer: 105°
The angle between the velocities V1 and V2 can be determined using the conservation of momentum and the relationship between the masses. Given that m1 is twice m2 and the final velocity of A is at a specific angle, the resulting velocity of B must be oriented such that the angle between them is 105°, ensuring momentum is conserved in both the x and y directions.
Answer: 8.75 × 10⁻⁴ J
For a solid sphere rolling without slipping, KE = (1/2)mv^2 + (1/2)Iw^2 = (7/10)mv^2. With m=0.5 kg and v=0.05 m/s, KE = 0.7*0.5*0.0025 = 8.75e-4 J.
Answer: mω²/k
The correct option, mω²/k, represents the relationship between the centripetal force required to keep the mass in circular motion and the restoring force of the spring. Since the spring's extension is directly proportional to the force applied, this formula accurately captures how the spring stretches under the influence of the rotational motion.
Answer: [2(m1 − m2)gh/((m1 + m2)R² + I)]^(1/2)
The correct option accounts for the net force acting on the system, which is the difference in weights of the two masses (m1 - m2), and incorporates the rotational inertia of the wheel. This results in a derived angular speed that reflects both the translational motion of the masses and the rotational motion of the wheel, ensuring energy conservation is maintained.
Answer: T = √(2πm/IB)
Restoring torque about the diameter is tau = -mu*B*sin(th) ~ -(I*pi*a^2)*B*th. With moment of inertia of the ring about a diameter = m*a^2/2, angular frequency^2 = mu*B/(m*a^2/2) = 2*pi*I*B/m. Hence T = 2*pi/sqrt(2*pi*I*B/m) = sqrt(2*pi*m/(I*B)).
Answer: (3/4) ((2a + b)/(3a + b)) L
With rho=a+b(x/L)^2: total mass = L(3a+b)/3 and integral of x*rho = L^2(2a+b)/4. So x_cm = [L^2(2a+b)/4]/[L(3a+b)/3] = (3/4)*((2a+b)/(3a+b))*L.