Dynamics of rotation about a fixed axis · Physics Class 11–12 | StemPy Lab
Course 6.2·Lesson 3 of 3
Dynamics of rotation about a fixed axis
For rotation about a fixed axis, Newton's second law becomes τ=Iα: the net torque equals the moment of inertia times the angular acceleration. A turning body has kinetic energy 21Iω2
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The law of rotation
For a body turning about a fixed axis, the turning version of F=ma is
τnet=Iα
Every straight-line idea has its turning twin:
Straight line
Turning about a fixed axis
mass m
moment of inertia I
force F
torque τ
F=ma
τ=Iα
kinetic energy 21mv2
21Iω2
work Fd
τθ
power Fv
τω
A rope on a drum
A mass m hangs from a rope wound round a drum of moment of inertia I and radius R. Two laws, one for each body, joined by the rope:
the mass: mg−T=ma;
the drum: TR=Iα;
the rope does not slip: a=αR.
For a solid drum, I=21MR2, and these give a=m+21Mmg. Explore it.
You should find that a heavy drum slows the fall a lot, and the tension then nearly equals the weight; a very light drum lets the mass fall almost freely, with almost no tension.
Watch out. The tension is not mg when the mass accelerates. Find it from the mass's own equation.
A worked example
A grindstone with I=0.50kg m2 is driven by a motor torque of 4.0N m against a friction torque of 1.0N m.