Table below given analogy between translational and rotational motions. Match the following.
Linear motion |
Relation motion |
velocity |
Angular momentum |
mass |
1/2 τω2 |
\(\frac{1}{2}\) mv2 |
τ = \(\frac{dL}{dt}\) |
a = \(\frac{dv}{dt}\) |
Moment of inertia |
F = \(\frac{dp}{dt}\) |
1/2 lω2 |
|
F = \(\frac{dl}{dt}\) |
|
Torque a =\(\frac{dω}{c^"}\) |