A **rigid body** is a system of particles in which the distance between the particles remains unchanged. It executes **plane motion** if all parts of the body moves in parallel planes.

A plane motion in which every line in the body remains parallel to its original position is called **translation**.

In a fixed axis rotation, all lines in the body which are perpendicular to the axis of rotation rotates through the same angle in same time. Thus, all lines on a body in its plane of motion have the same angular displacement ($\theta$), the same angular velocity ($\omega=\mathrm{d}\theta/\mathrm{d}t$), and the same angular acceleration ($\alpha=\mathrm{d}\omega/\mathrm{d}t$).

The angular velocity and the angular displacement of a body rotating in a plane with a **constant angular acceleration** $\alpha$ are given by
\begin{align}
&\omega=\omega_0+\alpha t, \nonumber\\
&\theta=\theta_0+\omega_0 t+\tfrac{1}{2}\alpha t^2, \nonumber\\
&\omega^2=\omega_0^2+2\alpha t, \nonumber
\end{align}
where $\theta_0$ and $\omega_0$ are angular displacement and angular velocity at time $t=0$.

In plane motion of a rigid body, the directions of angular velocity $\vec\omega$ and angular acceleration $\vec\alpha$ remains fixed (these are normal to the plane of rotation).

The velocities and accelerations of two points O and P on the rigid body are related by
\begin{align}
&\vec{v}_P=\vec{v}_O+\vec{\omega}\times{\vec{\mathrm{OP}}}=\vec{v}_O+\vec{\omega}\times\vec{r}, \nonumber\\
&\vec{a}_P=\vec{a}_O+\vec{\omega}\times\vec{\omega}\times\vec{r}+\vec{\alpha}\times\vec{r}, \nonumber
\end{align}
where $\vec{r}={\vec{\mathrm{OP}}}$ is the position vector from O to P. The acceleration term $\vec{\omega}\times\vec{\omega}\times\vec{r}$ is called **centripetal acceleration** and $\vec{\alpha}\times\vec{r}$ is called **tangential acceleration**.

If the axis of rotation is fixed then $\vec{v}_O=\vec{a}_O=\vec{0}$ for point O lying on the axis. This type of motion is called fixed axis rotation. In this case, the velocity of a point at a perpendicular distance $r$ from the axis is $v=\omega r$ (tangential). The centripetal acceleration of this point is $\omega^2 r$ and its tangential acceleration is $\alpha r$.

An axis perpendicular to the plane of rotation that passes through the point of zero instantaneous velocity (this point may or may not lie on the body) is called instantaneous axis of rotation.

If two points on a rigid body are instantaneously at rest then all points on the line joining these points is at rest (instantaneous axis of rotation). The angular velocity of the body at that instant is along this line.

The tangential component of velocity (i.e., component along the string) of any point on the string is same. Same is true for the acceleration.

Consider motion of a ball on a surface (fixed or moving). At the contact point, the ball may or may not slide on the surface. If tangential velocity of the ball at the contact point is equal to the velocity of the surface at this point then there is no slipping. Same is true for the acceleration.

- A disc is rolling (without slipping) on a horizontal surface (IIT JEE 2004)
- A sphere is rolling without slipping on a horizontal plane (IIT JEE 2009)
- The figure shows a system consisting of (IIT JEE 2012)
- Two identical discs of same radius R are rotating about their axes (IIT JEE 2012)
- The general motion of a rigid body can be considered to be a combination of (IIT JEE 2012)
- A Roller is Made by Joining Together Two Cones (JEE Mains 2016)

- Kinematics of Rigid Bodies
- Moment of Inertia
- Angular Momentum
- Angular Momentum of a Projectile
- Torque
- Conservation of Angular Momentum
- Fixed Axis of Rotation
- Rolling without slipping of rings cylinders and spheres
- Equilibrium of rigid bodies
- Direction of frictional force on bicycle wheels