Physics > Rotational Dynamics > 1.0 Introduction
Rotational Dynamics
1.0 Introduction
1.1 Torque or moment of a force
1.2 Relation between torque and moment of inertia
1.3 Pseudo torque
1.4 Torque equation
1.5 Principal of moments
2.0 Angular momentum or moment of a momentum
3.0 Relation between torque and angular momentum
4.0 Combined translational and rotational motion of a rigid body
5.0 Rotational kinetic energy
6.0 Uniform pure rolling
7.0 Accelerated pure rolling
8.0 Instantaneous axis of rotation
9.0 Toppling
1.4 Torque equation
1.2 Relation between torque and moment of inertia
1.3 Pseudo torque
1.4 Torque equation
1.5 Principal of moments
Torque equation is the vector sum of all the torques due to every force about an axis of rotation.
Let us consider a rigid body which is subjected to $n$ number of forces. These forces produces torque $\left( {{{\overrightarrow \tau }_1},{{\overrightarrow \tau }_2}...,{{\overrightarrow \tau }_n}} \right)$ about an axis of rotation as shown in the figure.
Mathematically, $${\overrightarrow \tau _{net}} = {\overrightarrow \tau _1} + {\overrightarrow \tau _2} + ... + {\overrightarrow \tau _n}$$
The net torque $\left( {{{\overrightarrow \tau }_{net}}} \right)$ produces an angular acceleration $\left( {\overrightarrow \alpha } \right)$ about an axis of rotation whose moment of inertia is $I$.
So, $${\overrightarrow \tau _{net}} = I\overrightarrow \alpha $$ or $$I\overrightarrow \alpha = {\overrightarrow \tau _1} + {\overrightarrow \tau _2} + ... + {\overrightarrow \tau _n}$$