Constrained Motion (Kinematic Linkages) — JEE Main Physics MCQs with Solutions
Free JEE Main Physics Constrained Motion (Kinematic Linkages) MCQs with step-by-step solutions (25 questions). Part of Newton's Laws of Motion & Friction. Practise online on Prepizo — no login needed.
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Questions with solutions
Q1 — Constrained Motion (Kinematic Linkages) · medium · theory
For an inextensible string connecting two bodies, the constraint condition is that:
A. The components of the velocities of its two ends along the string are equal ✓ Correct
B. The string tension is zero
C. The two ends have opposite accelerations of unequal magnitude
D. The velocities of the two ends are always equal in all directions
Solution: Inextensibility means the length is constant, so the rate at which the string is fed in at one end equals that at the other — i.e. equal velocity components along the string.
Q2 — Constrained Motion (Kinematic Linkages) · hard · theory
The virtual-work (constraint) method uses the fact that the total work done by the internal string tensions in an ideal system is:
A. Always positive
B. Equal to the change in kinetic energy
C. Zero ✓ Correct
D. Equal to the applied force times distance
Solution: For ideal (massless, inextensible) strings the net work of the tension pairs is zero: Σ T·v = 0, giving the acceleration/velocity constraint relations.
Q3 — Constrained Motion (Kinematic Linkages) · hard · theory
A load hangs from a single movable pulley and the free end of the string is pulled upward. The load moves:
A. At twice the speed of the free end
B. At half the speed of the free end ✓ Correct
C. At the same speed as the free end
D. In the opposite direction to the free end
Solution: A movable pulley is supported by two string segments, so the load moves half as fast (and half as far) as the free end. Pitfall: correspondingly the effort force is half the load.
Q4 — Constrained Motion (Kinematic Linkages) · medium · theory
The string-constraint equation for a system of connected bodies is obtained by requiring that:
A. The total mass is constant
B. The kinetic energy is constant
C. The total length of the (inextensible) string is constant, so the sum of the rates of change of its segments is zero ✓ Correct
D. The tension is the same as the weight
Solution: Differentiating "total length = constant" gives Σ(dℓ_i/dt) = 0 (and a second derivative gives the acceleration constraint).
Q5 — Constrained Motion (Kinematic Linkages) · hard · theory
A block slides on the incline of a wedge that is itself free to move on the floor. The constraint is that:
A. The block's absolute acceleration is along the incline
B. The block cannot move relative to the wedge
C. The block's acceleration relative to the wedge is directed along the incline surface ✓ Correct
D. The wedge must remain stationary
Solution: The block stays in contact with the wedge, so its acceleration relative to the wedge lies along the incline; its absolute acceleration is the vector sum of that and the wedge's acceleration.
Q6 — Constrained Motion (Kinematic Linkages) · medium · theory
For two blocks connected by a single inextensible string over a fixed ideal pulley, the magnitudes of their accelerations are:
A. Inversely proportional to their masses
B. Equal ✓ Correct
C. In the ratio of their masses
D. Always zero
Solution: A single string over a fixed pulley gives both blocks the same speed and the same magnitude of acceleration.
Q7 — Constrained Motion (Kinematic Linkages) · hard · theory
For a rigid rod, the constraint linking the velocities of its two ends A and B is:
A. The rod length changes with time
B. The components of v_A and v_B along the rod are equal ✓ Correct
C. v_A = v_B in magnitude and direction
D. v_A and v_B are perpendicular
Solution: A rigid rod cannot stretch, so the velocity components of its two ends along the rod must be equal.
Q8 — Constrained Motion (Kinematic Linkages) · medium · theory
A block rests on a wedge that can slide on the ground. If the wedge accelerates, the block's motion is constrained by:
A. Both the contact with the incline and (if applicable) the string over the wedge pulley ✓ Correct
B. No constraint at all
C. Only the normal reaction
D. Only gravity
Solution: Contact with the wedge surface (and any connecting string) provides the geometric constraints that relate the block's and wedge's accelerations.
Q9 — Constrained Motion (Kinematic Linkages) · hard · theory
An ideal movable-pulley arrangement in which the load is supported by n string segments gives a mechanical advantage (ideal) of:
A. 1
B. 1/n
C. n²
D. n ✓ Correct
Solution: With n supporting segments, the effort = load/n, so the ideal mechanical advantage is n (velocity ratio is also n).
Q10 — Constrained Motion (Kinematic Linkages) · medium · theory
In the virtual-work method, one assigns small virtual displacements to the bodies that are:
A. Always equal for all bodies
B. Consistent with the constraints, then sets the net work of the constraint forces to zero ✓ Correct
C. Arbitrary and unrelated to the constraints
D. Perpendicular to all forces
Solution: Virtual displacements must respect the constraints; since constraint forces do no net work, ΣF·δr for the active forces gives the required relation.
Q11 — Constrained Motion (Kinematic Linkages) · medium · numerical
Two blocks are connected by a string over a fixed ideal pulley. If one block descends at 3 m/s, the other block:
A. Rises at 1.5 m/s
B. Rises at 3 m/s ✓ Correct
C. Stays at rest
D. Rises at 6 m/s
Solution: Single string over a fixed pulley ⇒ equal speeds. The other block rises at 3 m/s.
Q12 — Constrained Motion (Kinematic Linkages) · medium · numerical
A load hangs from a movable pulley whose string's free end is pulled upward at 6 m/s. The load rises at:
A. 1.5 m/s
B. 6 m/s
C. 12 m/s
D. 3 m/s ✓ Correct
Solution: Movable pulley ⇒ load speed = half the free-end speed = 6/2 = 3 m/s.
Q13 — Constrained Motion (Kinematic Linkages) · medium · numerical
A load on a movable pulley rises at 2 m/s. The free end of the string is being pulled at:
A. 8 m/s
B. 4 m/s ✓ Correct
C. 1 m/s
D. 2 m/s
Solution: Free-end speed = 2 × load speed = 2 × 2 = 4 m/s.
Q14 — Constrained Motion (Kinematic Linkages) · medium · numerical
In an ideal single-movable-pulley system, the effort needed to just support a 200 N load is:
A. 200 N
B. 100 N ✓ Correct
C. 400 N
D. 50 N
Solution: Two supporting segments ⇒ effort = load/2 = 200/2 = 100 N.
Q15 — Constrained Motion (Kinematic Linkages) · hard · numerical
A ladder leans against a wall. Its foot (end A) slides along the floor at 5 m/s. When the ladder makes 37° with the floor (sin37° = 0.6, cos37° = 0.8), the top end B slides down at:
A. 5 m/s
B. ≈ 4 m/s
C. ≈ 3.75 m/s
D. ≈ 6.67 m/s ✓ Correct
Solution: Equal velocity components along the rod: v_A cosθ = v_B sinθ ⇒ v_B = v_A cotθ = 5 × (0.8/0.6) ≈ 6.67 m/s.
Q16 — Constrained Motion (Kinematic Linkages) · hard · numerical
A ladder's foot slides at 4 m/s along the floor. When the ladder makes 53° with the floor (cot53° = 0.75), the speed of its top end (on the wall) is:
A. 6 m/s
B. 3 m/s ✓ Correct
C. 4 m/s
D. 5.33 m/s
Solution: v_B = v_A cotθ = 4 × 0.75 = 3 m/s.
Q17 — Constrained Motion (Kinematic Linkages) · hard · numerical
A block on the floor is pulled by a rope passing over an overhead pulley; the rope is drawn in at 5 m/s and makes 60° with the horizontal at the block. The speed of the block is:
A. 10 m/s ✓ Correct
B. 5 m/s
C. ≈ 8.7 m/s
D. 2.5 m/s
Solution: Rate of shortening of the rope = component of block velocity along the rope: 5 = v cos60° ⇒ v = 5/0.5 = 10 m/s. Pitfall: the block moves faster than the rope is pulled.
Q18 — Constrained Motion (Kinematic Linkages) · hard · numerical
A block is dragged by a rope over a pulley, the rope being pulled in at 6 m/s while it makes 30° with the block's (horizontal) motion. The block's speed is (cos30° ≈ 0.866):
A. ≈ 6.93 m/s ✓ Correct
B. ≈ 5.2 m/s
C. 3 m/s
D. 12 m/s
Solution: 6 = v cos30° ⇒ v = 6/0.866 ≈ 6.93 m/s.
Q19 — Constrained Motion (Kinematic Linkages) · medium · numerical
Two blocks connected by a string over a fixed pulley: one has a downward acceleration of 4 m/s². The other block's acceleration is:
A. 2 m/s² upward
B. 4 m/s² upward ✓ Correct
C. 8 m/s² upward
D. 4 m/s² downward
Solution: Single string, fixed pulley ⇒ equal-magnitude accelerations in opposite senses: 4 m/s² upward.
Q20 — Constrained Motion (Kinematic Linkages) · hard · numerical
The free end of the string of a movable-pulley system is pulled with an acceleration of 8 m/s². The load's acceleration is:
A. 4 m/s² ✓ Correct
B. 2 m/s²
C. 8 m/s²
D. 16 m/s²
Solution: Load acceleration = half the free-end acceleration = 8/2 = 4 m/s².
Q21 — Constrained Motion (Kinematic Linkages) · medium · numerical
A block on a smooth table is joined by a string over an edge pulley to a hanging block. If the hanging block accelerates down at 3 m/s², the table block accelerates horizontally at:
A. 1.5 m/s²
B. 6 m/s²
C. 0
D. 3 m/s² ✓ Correct
Solution: A single inextensible string over one pulley forces equal accelerations: 3 m/s².
Q22 — Constrained Motion (Kinematic Linkages) · hard · numerical
Two blocks are joined by a rigid rod inclined at 37° to the horizontal. Block A moves horizontally at 10 m/s and block B moves vertically. The speed of B is (sin37° = 0.6, cos37° = 0.8):
A. ≈ 6 m/s
B. 10 m/s
C. ≈ 13.3 m/s ✓ Correct
D. ≈ 7.5 m/s
Solution: Equal components along the rod: v_A cos37° = v_B cos53° ⇒ 10 × 0.8 = v_B × 0.6 ⇒ v_B = 8/0.6 ≈ 13.3 m/s.
Q23 — Constrained Motion (Kinematic Linkages) · hard · numerical
A block moves horizontally at 8 m/s while a rope attached to it (going up to a pulley) makes 60° with the horizontal. The rate at which the rope is being shortened (pulled in) is:
A. ≈ 6.9 m/s
B. 4 m/s ✓ Correct
C. 8 m/s
D. 16 m/s
Solution: Rate of shortening = v cos60° = 8 × 0.5 = 4 m/s (the component of the block's velocity along the rope).
Q24 — Constrained Motion (Kinematic Linkages) · hard · numerical
In an ideal pulley system where the load is supported by 3 string segments, the effort needed to just hold a 300 N load is:
A. 900 N
B. 300 N
C. 100 N ✓ Correct
D. 150 N
Solution: Effort = load/n = 300/3 = 100 N (ideal mechanical advantage 3).
Q25 — Constrained Motion (Kinematic Linkages) · medium · numerical
A ladder makes 45° with the floor. If its foot slides out at 2 m/s, the top slides down at:
A. 2 m/s ✓ Correct
B. ≈ 2.8 m/s
C. 4 m/s
D. 1 m/s
Solution: v_B = v_A cot45° = 2 × 1 = 2 m/s (equal at 45°).