A-Level Physics AQA 7408

11.1: Rotational dynamics

#11.1.1

Concept of moment of inertia

I=mr2I = mr^2 for a point mass.

I=Σmr2I = Σmr^2 for an extended object.

Qualitative knowledge of the factors that affect the moment of inertia of a rotating object.

Expressions for moment of inertia will be given where necessary.

#11.1.2

Rotational kinetic energy

Ek=12Iω2E_k = \dfrac{1}{2}Iω^2

Factors affecting the energy storage capacity of a flywheel.

Use of flywheels in machines.

Use of flywheels for smoothing torque and speed, and for storing energy in vehicles, and in machines used for production processes.

#11.1.3

Rotational motion

Angular displacement, angular speed, angular velocity, angular acceleration, ω=θtω = \dfrac{∆θ}{∆t} , α=ωtα = \dfrac{∆ω}{∆t}

Representation by graphical methods of uniform and non-uniform angular acceleration.

Equations for uniform angular acceleration;

ω2=ω1+αtω_2 = ω_1 + αt, θ=(ω1+ω22)tθ = \Big(\dfrac{ω_1+ω_2}{2}\Big)t

θ=ω1t+αt22θ = ω_1t + \dfrac{αt^2}{2} , ω22=ω12+2αθω_2^2 = ω_1^2 + 2αθ

Students should be aware of the analogy between rotational and translational dynamics.

#11.1.4

Torque and angular acceleration

T=FrT = Fr

T=IαT = Iα

#11.1.5

Angular momentum

angular momentum=Iω\text{angular momentum} = Iω

Conservation of angular momentum.

Angular impulse = change in angular momentum; Tt=(Iω)T∆t=∆(Iω) where T is constant.

Applications may include examples from sport.

#11.1.6

Work and power

W=TθW = Tθ ; P=TωP = Tω

Awareness that frictional torque has to be taken into account in rotating machinery.

10.6
Radionuclide imaging and therapy
11.2
Thermodynamics and engines