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F&C ch 8
Consider an object rotating about the origin in the x-y plane with angular velocity w. Let's pick a point on the body, labelled by i, at location ri = ricosq i + risinq j = xi i + yi j . This point will have a velocity vi which must be perpendicular to ri and a magnitude of vi = wri such that we can write vi = -vi sinq i + vi cosq j = w(-ri sinq i + ri cosq j) = w(-yi i + xi j). But if we say that angular velocity is a vector -- and why not, both velocity and angular momentum are vectors -- then writing w = wk, we see that wŚri = w(-yi i + xi j) = vi.
relation | translational motion | rotational motion |
momentum | px = mvx | Lz = Izw |
kinetic energy | T = 1/2 mv2 | T = 1/2 Izw |
equation of motion | Fx = dpx/dt | Nz = dLz/dt |
© 11 March 1999 R. Harr