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Dynamics cheat sheet

my dynamics notes - 12000.org

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11 Formulas<br />

sin 2 x 1cos2x<br />

2<br />

cos 2 x 1cos2x<br />

2<br />

sin 2x 2 sin x cosx<br />

cos2x cos 2 x sin 2 x<br />

1 2 sin 2 x<br />

V p V o r V rel<br />

Velocity of p<br />

relative to o<br />

a p a 0 r r 2 V rel a rel<br />

p<br />

IF rigid body is rotating AND translation at the same time THEN<br />

Take moments around its cg only<br />

ELSE<br />

can also take moments about any other points on it (but<br />

change I)<br />

END IF<br />

o<br />

r<br />

<br />

Y<br />

R Y<br />

X<br />

R y<br />

R X<br />

R<br />

x<br />

y<br />

<br />

R x<br />

BODY FIXED<br />

COORDINATES<br />

This gives the relation<br />

between the rate of<br />

change with respect to<br />

time of a vector expressed<br />

in a frame of reference<br />

which is body fixed (y,x)<br />

here, to the rate of change<br />

with respect to time of the<br />

same vector expressed<br />

using an inertial frame<br />

coordinates XY.<br />

The omega here is the<br />

angular velocity of the<br />

rigid body rotation, or the<br />

body fixed coordinates,<br />

with respect to the inertial<br />

frame.<br />

d<br />

dt R X,Y d dt R x,y R X,Y<br />

<br />

R<br />

r<br />

<br />

R r<br />

r<br />

The small disk rotates<br />

at angular speed of <br />

The condition of no slip can<br />

be seen to be<br />

R r r<br />

For the sign of generalized force:<br />

If work done by force takes away<br />

energy from system, then the<br />

sign is negative, else positive. So<br />

Friction will always have negative<br />

sign, so will damping force.<br />

d<br />

dt<br />

cosxt sinxtx t<br />

d<br />

dt<br />

df<br />

dxt<br />

<br />

d<br />

dxt<br />

d<br />

cosxt <br />

dt<br />

df<br />

dxt<br />

d<br />

d<br />

cos xt<br />

dxt<br />

d<br />

xt dt<br />

xt dt<br />

51

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