### Angular Momentum & Moment of Inertia for Rotational Motion

##### November 20, 2017

# Angular Momentum

In our last post we have discussed on **Linear momentum**. Just to brush up, when an object of mass *m *moves with a speed *v *in a straight line, we say that it has a linear momentum, **p=mv.** When the same object moves with an angular speed **ω** along the circumference of a circle of radius *r*, then we say that it has an **angular momentum**, ** L**. This

*depends on 2 quantities, one is*

**L****rotational inertia**or

**moment of inertia**and the other one is

**angular velocity**. Let’s discuss in details till we get the concept of

**torque**.

## Inertia vs Moment of Inertia

Linear momentum or simply momentum is a product of mass and linear velocity. And you know, this mass is the determining factor of inertia (property of an object to retain its state of motion – when either it’s moving linearly or in static condition), that’s why mass is also called **inertia** for linear motion.

If we try to find out the **equivalent of linear inertia for the rotational motion** then we get the notion of **Rotational Inertia**. Here comes Newton’s first law which is also called the law of inertia. This law applies to rotating objects as well. When an object is rotating about an internal axis, the object tends to keep rotating about that axis. Rotating objects tend to continue its rotating and non-rotating objects tend to remain non-rotating.

An object resists to changes in its rotational motion. This resistance is called **rotational inertia** (or the **moment of inertia**).The greater an object’s rotational inertia, the more difficult it is to change the rotational speed of the object.

A force is required to change the linear state of motion of an object. Similarly a torque is required to change the rotational state of motion of an object. In the absence of a net torque, a rotating object keeps rotating, while a non-rotating one stays non-rotating. **This moment of inertia is designated with the sign I.**

## Equation of Angular Momentum

The magnitude of **angular momentum*** L *is given by replacing *m *and *v *in the expression for linear momentum *p *with their angular analogues ** I **and

**ω.**[ I is the moment of inertia or rotational inertia and ω is the angular velocity]

Thus we express the angular momentum as follows: *L = I ω ………………… (1)*

SI unit of angular momentum:kg.m^2/s

This expression is applicable to any object undergoing angular motion, whether it is a point mass moving in a circle or a rotating disk.

## Definition of the Angular Momentum

Angular momentum L is defined as the product of rotational inertia, **I**, and rotational velocity, **ω** .

**angular momentum(L) = rotational inertia (I) .** **rotational velocity (ω)**

Like linear momentum, angular momentum is a vector quantity and has direction as well as magnitude.

## Angular Momentum for a point mass

Now let’s say a point mass *m *moving in a circle of radius *r.
* The moment of inertia varies for different shapes and in this case for a point mass it is I=mr^2.

In addition to this, the linear speed of the mass is **v=ωr**. [Ref: our **post** on linear motion and circular motion – 3 relations]

That means, **ω = v/r**

Combining these results **for a point mass**, we find *L = I ω =(mr^2) (v/r) = rmv…………….. (2)*

Noting that *mv *is the linear momentum *p*, we find that the angular momentum of a point mass can be written in the following form:

**L =rmv =r p ………………….. (3)**

It is important to recall that these 2 expressions (equation 2 and 3) apply specifically to a **point particle** moving along the circumference of a circle.

## Rate of change of Angular Momentum with Time – Torque

Rate of change of Angular Momentum with respect to time = ΔL/ΔT

Now, ΔL/ΔT = Δ(I ω)/ΔT = I. Δω/ΔT ……. (4) [ Here I is constant when mass and shape of the object are unchanged]

Now Δω/ΔT is the rate of change of angular velocity with time i.e. angular acceleration (α).

So from equation 4 we can write, ΔL/ΔT = I α …………………(5)

Have you noticed this I α ? I (moment of inertia) is the rotational equivalent of mass(inertia) of linear motion. Similarly α (alpha) is the rotational motion equivalent of a (linear acceleration).

As in combined (product) form m and a represents Force in linear motion, similarly I and α in product form represent **Torque (τ)**, which in turn is the rotational equivalent of Force.

So from equation 5 we get, ΔL/ΔT = τ ……………………. (6)

**Definition of Torque**: Thus we can state that the torque can be expressed as the rate of change in angular momentum with time.

Related study: **Linear Momentum**

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