**Chapter 4: RIGID BODIES III
**

**ROTATION. CIRCULAR MOTION.****MOMENT OF A FORCE (TORQUE).****MOMENT ANGULAR CONSERVATION.**

**Massachusetts Institute of Technology** have developed Open Course Wares (OCW) where you can follow a “**Classical Mechanics course**” by Internet.

One of the most important magnitudes in architecture is the **moment of a force** or **torque**. And this magnitude will be extremely important in **Chapter 5: Equilibrium**.

Linear momentum, i.e. **p = **m**·v**, has a rotational analogue that it is called **angular momentum**, **L**. For a symmetrical object rotating about a fixed axis through the centre of mass (CM), the angular momentum is **L =** I**·ω** where I is the moment of inertia and **ω** is the angular velocity about the axis of rotation. The SI units for L are **kg·m^2/s**, which has no special name.

We saw in **Chapter 2: Dynamics laws and applications** that **Newton’s second law** can be written more generally in terms of momentum Σ**F** = Δ**p**/Δt. In a similar way, the rotational equivalent of Newton’s second law which is Σ**τ** = I·**α**, can also be written more generally in terms of angular momentum Σ**τ** = Δ**L**/Δt where Σ**τ** is the net torque acting to rotate the object and Δ**L** is the change in angular momentum in a interval time Δt.

**Angular momentum** is an important concept in physics because, **under certain conditions**, it is a **conserved** quantity. If Σ**τ** = Δ**L**/Δt on an object is zero then Δ**L** = 0, so **L** does not change. This is the **law of conservation of angular momentum** for a rotating object:

**The total angular momentum of a rotating object remains constant if the net torque acting on it is zero.**

- A video tutorial about
**rotation**can be watched on the MIT-OCW webpage:

- A video tutorial about the
**moment of a force/torque**can be watched on the MIT-OCW webpage:

- A video tutorial about
**rotational dynamics**can be watched on the MIT-OCW webpage:

- A video tutorial about
**solved problems**can be watched on the MIT-OCW webpages:

Worked example: moment-of-inertia-of-a-disc-from-a-falling-mass

Worked example: massive-pulley-problems

**MisConceptual Questions**

- The symmetric simple truss is loaded as shown in Figure. Which force shown exerts the largest magnitude torque on the truss around point A? And around point B?
- Calculate the net torque around point O due to the forces acting on the plate shown.

**Video lecture: Rotational dynamic example
**

**Problem set number 5**

- A wheel of radius
**r = 80 cm**has moment of inertia**10 kg·m^2**. It is rotating around its central axis propelled by a rocket attached to a point on its outer rim. The rocket is expelling gas

tangentially to the wheel, resulting in a constant force. Determine:- The magnitude of the equivalent force, if we know that the wheel, starting from rest, reaches an angular speed of
**1 rev/s**in 6 s. - The value of both tangential and normal acceleration in a point on the outer rim of the wheel.
- The angle that the total acceleration forms with the radius at that point.
- The time that the wheel takes to reach the same angular velocity, under the action of the same force, if we add a very thin ring of mass
**5 kg**around the outer rim.

- The magnitude of the equivalent force, if we know that the wheel, starting from rest, reaches an angular speed of

If you have some doubts, you can watch next video related to rotational dynamic (**Professor Michel van Biezen**):

If you were satisfied with this example, you can check more video lectures on the webpage: