NCERT Class XI · Physics · Chapter 3

Motion in a Plane True–False Lab

Use this dedicated True–False set to stress‑test your understanding of vectors, projectile motion, relative velocity and uniform circular motion before attempting full‑length numericals or JEE/NEET‑level questions.

Scalars vs Vectors Dot & Cross Products Projectile Motion Formulae Uniform Circular Motion Relative Motion & River–Boat
Start the True–False Challenge 25 conceptual statements covering vectors, parabolic trajectories, UCM and relative velocity – mark T/F then justify each in one line.
Concept
Integrity
Check
Vectors & Components
Projectile Motion
Circular Motion
Chapter Snapshot
Motion in a Plane brings 1D kinematics into two dimensions using vectors, and underpins projectile motion, relative motion and uniform circular motion.
Why True–False?
Best Use
Scalars, Vectors & Components

Distinguish scalar vs vector quantities, test when vectors are equal, and practise resolving any vector into unique components along chosen perpendicular axes. Many statements here probe sign conventions and “perpendicular / parallel” logic via dot and cross products.

Dot & Cross Products

Use \(\vec{A}\cdot\vec{B}=AB\cos\theta\) to detect perpendicularity and projections, and \(|\vec{A}\times\vec{B}|=AB\sin\theta\) plus the right‑hand rule for area and direction. Several True–False items hinge on recognising when these products vanish or become maximum.

Projectile Motion & Parabolic Path

Horizontal velocity component stays constant; vertical component changes uniformly under gravity, giving a parabolic trajectory on level ground. Statements about time of flight, range, complementary angles and “same height” speeds are designed to check your grasp of these standard results.

Uniform Circular Motion

In UCM, speed is constant but velocity and acceleration directions keep changing; acceleration is \(v^{2}/r\) toward the centre and tangential acceleration is zero. Some statements test how centripetal acceleration scales when speed or radius are changed.

Relative Velocity & River–Boat

Relative velocity \(\vec{v}_{BA} = \vec{v}_B - \vec{v}_A\) governs rain‑man and river‑boat problems. The True–False questions here ensure you can reason about shortest time vs shortest path and interpret “velocity of A with respect to B” correctly.

How to Use This True–False Set for Maximum Gain

Ready? Scroll down to the True–False questions list below and start with: “A physical quantity that has only magnitude and no direction is called a scalar” and continue through projectiles, circular motion and relative velocity. Treat each as a mini concept‑check before you move to numericals.
Your Progress 0 / 25 attempted
Q 01 / 25
A body can remain in uniform motion even when several forces act on it simultaneously.
Q 02 / 25
In an inertial frame, if the net external force on a particle is zero, its acceleration must be zero.
Q 03 / 25
Newton’s third law implies that the forces in an action–reaction pair always act on the same body.
Q 04 / 25
The frictional force on a body is always opposite to its velocity.
Q 05 / 25
Static friction can adjust its magnitude up to a certain maximum value.
Q 06 / 25
A car moving on a straight road with constant speed is in mechanical equilibrium.
Q 07 / 25
If a resultant force acts on a body, its speed must change.
Q 08 / 25
Tension in a light, inextensible string is the same at all points in one straight segment in equilibrium.
Q 09 / 25
Normal reaction exerted by a horizontal surface on a resting block is always equal to the weight of the block.
Q 10 / 25
In an action–reaction pair, forces are equal and opposite but may not balance each other in a free-body diagram.
Q 11 / 25
The coefficient of friction between two surfaces depends on the apparent area of contact.
Q 12 / 25
In uniform circular motion on a horizontal road, static friction provides the necessary centripetal force.
Q 13 / 25
The pseudo force on a mass \(m\) in a linearly accelerating frame of acceleration \(\vec{a}\) is \(-m\vec{a}\).
Q 14 / 25
Newton’s laws of motion hold exactly in any frame moving with constant velocity relative to the “fixed stars”.
Q 15 / 25
The kinetic friction on a sliding block always equals \(\mu_k N\), independent of its speed (within moderate speeds).
Q 16 / 25
In a system of two blocks connected by a light string on a smooth surface, internal tension forces can change the total linear momentum of the system.
Q 17 / 25
For a block in an accelerating lift, the apparent weight equals the normal reaction exerted by the floor on the block.
Q 18 / 25
During a collision of two isolated bodies in one dimension, the total momentum is conserved even if the collision is inelastic.
Q 19 / 25
A system moving under the action of only internal forces cannot have a changing centre-of-mass velocity.
Q 20 / 25
In a pulley system with a light, frictionless pulley and light string, the acceleration of all masses must be equal in magnitude.
Q 21 / 25
In a wedge–block system without friction, if the wedge is free to move on a smooth horizontal surface, the horizontal component of the normal between block and wedge is an internal force of the block–wedge system.
Q 22 / 25
For a bead constrained to move on a frictionless circular wire fixed in a car turning on a horizontal road, the normal reaction of the wire on the bead is the only real force responsible for changing the bead’s speed in the car’s frame.
Q 23 / 25
If the net external force on a system is always parallel to its velocity, the speed of the centre of mass must change but its direction of motion cannot change.
Q 24 / 25
In a rod of negligible mass pushing two unequal masses on a smooth surface, the internal forces on the rod at its two ends must be equal in magnitude.
Q 25 / 25
For any planar system of particles, if the vector sum of external forces is zero, then the system must be in static equilibrium.
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