Difficulty distribution
How the classified questions are distributed by difficulty.
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Practice Rotational Motion - Mechanics - Physics previous year questions organised from real papers, with year-wise coverage and clear topic navigation.
Every graph below is calculated only from this selection.
Year-wise coverage for Rotational Motion. Each bar uses a separate theme-derived color.
How the classified questions are distributed by difficulty.
MCQ, numerical, multiple-select and other formats found in these papers.
Top subjects by unique question coverage.
Top topics across the included previous year papers.
Top subtopics inside this exact selection.
Question coverage for the most populated papers. Every active PYP paper remains listed below.
Newest papers appear first. Sort by year, question coverage or name.
| Paper | Year / session | Questions in this view | Open |
|---|---|---|---|
| MHT CET 2026 11th April Evening Shift | 2026 | 2 | View paper |
| MHT CET 2026 11th April Morning Shift | 2026 | 2 | View paper |
| MHT CET 2026 13th April Evening Shift | 2026 | 3 | View paper |
| MHT CET 2026 13th April Morning Shift | 2026 | 2 | View paper |
| MHT CET 2026 15th April Morning Shift | 2026 | 2 | View paper |
| MHT CET 2026 16th April Evening Shift | 2026 | 3 | View paper |
| MHT CET 2026 16th April Morning Shift | 2026 | 1 | View paper |
| MHT CET 2026 17th April Evening Shift | 2026 | 3 | View paper |
| MHT CET 2026 17th April Morning Shift | 2026 | 3 | View paper |
| MHT CET 2026 18th April Evening Shift | 2026 | 3 | View paper |
| MHT CET 2026 18th April Morning Shift | 2026 | 3 | View paper |
| MHT CET 2026 19th April Evening Shift | 2026 | 1 | View paper |
| MHT CET 2026 19th April Morning Shift | 2026 | 2 | View paper |
| MHT CET 2026 20th April Evening Shift | 2026 | 1 | View paper |
| MHT CET 2026 20th April Morning Shift | 2026 | 3 | View paper |
| MHT CET (PCB) 2025 9th April Evening Shift | 2025 | 1 | View paper |
| MHT CET (PCB) 2025 9th April Morning Shift | 2025 | 2 | View paper |
| MHT CET 2025 19TH APRIL EVENING SHIFT | 2025 | 1 | View paper |
| MHT CET 2025 19TH APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 20TH APRIL EVENING SHIFT | 2025 | 2 | View paper |
| MHT CET 2025 20TH APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 21ST APRIL EVENING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 21ST APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 22ND APRIL EVENING SHIFT | 2025 | 2 | View paper |
| MHT CET 2025 22ND APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 23RD APRIL EVENING SHIFT | 2025 | 1 | View paper |
| MHT CET 2025 25TH APRIL EVENING SHIFT | 2025 | 4 | View paper |
| MHT CET 2025 25TH APRIL MORNING SHIFT | 2025 | 2 | View paper |
| MHT CET 2025 26TH APRIL EVENING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 26TH APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 5TH MAY EVENING SHIFT | 2025 | 2 | View paper |
| MHT CET (PCB) 2024 22th April Evening Shift | 2024 | 2 | View paper |
| MHT CET (PCB) 2024 22th April Morning Shift | 2024 | 2 | View paper |
| MHT CET 2024 10TH MAY EVENING SHIFT | 2024 | 1 | View paper |
| MHT CET 2024 10TH MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 11TH MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 11TH MAY MORNING SHIFT | 2024 | 1 | View paper |
| MHT CET 2024 15TH MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 15TH MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 16TH MAY EVENING SHIFT | 2024 | 1 | View paper |
| MHT CET 2024 16TH MAY MORNING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 2ND MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 2ND MAY MORNING SHIFT | 2024 | 1 | View paper |
| MHT CET 2024 3RD MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 3RD MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 4TH MAY EVENING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 4TH MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 9TH MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 9TH MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2023 10TH MAY EVENING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 10TH MAY MORNING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 11TH MAY EVENING SHIFT | 2023 | 2 | View paper |
| MHT CET 2023 11TH MAY MORNING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 12TH MAY EVENING SHIFT | 2023 | 2 | View paper |
| MHT CET 2023 12TH MAY MORNING SHIFT | 2023 | 2 | View paper |
| MHT CET 2023 13TH MAY EVENING SHIFT | 2023 | 2 | View paper |
| MHT CET 2023 13TH MAY MORNING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 14TH MAY EVENING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 14TH MAY MORNING SHIFT | 2023 | 1 | View paper |
| MHT CET 2023 9TH MAY EVENING SHIFT | 2023 | 1 | View paper |
| MHT CET 2023 9TH MAY MORNING SHIFT | 2023 | 3 | View paper |
| MHT CET 2021 20TH SEPTEMBER EVENING SHIFT | 2021 | 2 | View paper |
| MHT CET 2021 20TH SEPTEMBER MORNING SHIFT | 2021 | 3 | View paper |
| MHT CET 2021 21TH SEPTEMBER EVENING SHIFT | 2021 | 2 | View paper |
| MHT CET 2021 21TH SEPTEMBER MORNING SHIFT | 2021 | 2 | View paper |
| MHT CET 2021 22TH SEPTEMBER EVENING SHIFT | 2021 | 3 | View paper |
| MHT CET 2021 22TH SEPTEMBER MORNING SHIFT | 2021 | 2 | View paper |
| MHT CET 2021 23RD SEPTEMBER EVENING SHIFT | 2021 | 4 | View paper |
| MHT CET 2021 23th September Morning Shift | 2021 | 3 | View paper |
| MHT CET 2021 24TH SEPTEMBER EVENING SHIFT | 2021 | 1 | View paper |
| MHT CET 2021 24TH SEPTEMBER MORNING SHIFT | 2021 | 2 | View paper |
| MHT CET 2020 16TH OCTOBER EVENING SHIFT | 2020 | 3 | View paper |
| MHT CET 2020 16TH OCTOBER MORNING SHIFT | 2020 | 2 | View paper |
| MHT CET 2020 19TH OCTOBER EVENING SHIFT | 2020 | 3 | View paper |
| MHT CET 2019 2ND MAY EVENING SHIFT | 2019 | 4 | View paper |
| MHT CET 2019 2ND MAY MORNING SHIFT | 2019 | 4 | View paper |
| MHT CET 2019 3RD MAY MORNING SHIFT | 2019 | 2 | View paper |
Practice every matching question in batches of 20, with every available option.
A rigid body is rotating with angular velocity ' $\omega$ ' about an axis of rotation. Let $v$ ' be the linear velocity of particle which is at perpendicular distance ' $r$ ' from the axis of rotation. Then the relation $v=r \omega$ ' implies that
Three point masses each of mass ' $m$ ' are kept at the corners of an equilateral triangle of side. The system rotates about the center of the triangle without any change in the separation of masses during rotation. The period of rotation is directly proportional to $\left(\cos 30^{\circ}=\sin 60^{\circ}=\frac{\sqrt{3}}{2}\right)$
Three identical rods each of mass ' $M$ ' and length ' $L$ ' are joined to form a symbol ' $H$. The moment of inertia of the system about one of the sides of ' $H$ ' is
When a 12000 joule of work is done on a flywheel, its frequency of rotation increases from 10 Hz to 20 Hz . The moment of inertia of flywheel about its axis of rotation is $\left(\pi^2=10\right)$
If radius of the solid sphere is doubled by keeping its mass constant, the ratio of their moment of inertia about any of its diameter is
The dimensions of torque are same as that of
A uniform rod of length ' 6 L ' and mass ' 8 m ' is pivoted at its centre ' $C$ '. Two masses ' $m$ ' and ' $2 m^{\prime}$ with speed $2 v, v$ as shown strikes the rod and stick to the rod. Initially the rod is at rest. Due to impact, if it rotates with angular velocity ' $\omega$ ' then ' $\omega$ ' will be

A thin metal wire of length 'L' and uniform linear mass density '$\rho$' is bent into a circular coil with 'O' as centre. the moment of inertia of a coil about the axis XX' is

A solid sphere rolls down from top of inclined plane, 7 m high, without slipping. Its linear speed at the foot of plane is $\left(g=10 \mathrm{~m} / \mathrm{s}^2\right)$
A rod $l \mathrm{~m}$ long is acted upon by a couple as shown in the figure. The moment of couple is $\tau \mathrm{~Nm}$. If the force at each end of the rod, then magnitude of each force is
$$\left(\sin 30^{\circ}=\cos 60^{\circ}=0.5\right)$$

A body slides down a smooth inclined plane having angle \(\theta\) and reaches the bottom with velocity \(v\). If a body is a sphere, then its linear velocity at the bottom of the plane is
The ratio of radii of gyration of a ring to a disc (both circular) of same radii and mass, about a tangential axis perpendicular to the plane is
A thin uniform rod has mass \(M\) and length \(L\) The moment of inertia about an axis perpendicular to it and passing through the point at a distance \(\frac{L}{3}\) from one of its ends, will be
If there is a change of angular momentum from \(1 \mathrm{j}\)-\(\mathrm{s}\) to \(4 \mathrm{j}\)-\(\mathrm{s}\) in \(4 \mathrm{~s}\), then the torque
A solid cylinder of radius \(r\) and mass \(M\) rolls down an inclined plane of height \(h\). When it reaches the bottom of the plane, then its rotational kinetic energy is (\(g=\) acceleration due to gravity)
A rope is wound around a solid cylinder of mass 1 kg and radius 0.4 m . What is the angular acceleration of cylinder, if the rope is pulled with a force of 25 N ? (Cylinder is rotating about its own axis.)
Three points masses, each of mass $m$ are placed at the corners of an equilateral triangle of side $\ell$. The moment of inertia of the system about an axis passing through one of the vertices and parallel to the side joining other two vertices, will be
Two circular loop $A$ and $B$ of radii $R$ and $N R$ respectively are made from a uniform wire. Moment of inertia of $B$ about its axis is 3 times that of $A$ about its axis. The value of $N$ is
The ratio of radii of gyration of a circular ring and circular disc of the same mass and radius, about an axis passing through their centres and perpendicular to their planes is
A disc of radius 0.4 metre and mass 1 kg rotates about an axis passing through its centre and perpendicular to its plane. The angular acceleration is 10 rad s\(^{-2}\). The tangential force applied to the rim of the disc is
Showing 20 of 180 questions