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Circular uniform motion
Ac=V²/r
Fc=mv²/r or F=m(ac)
ac is proportional to r because v=w*r
Velocity perpindicular to centripetal force vector
Torque
t=rFsin(theta)
As r decreases F goes up: Smaller radius closer to pivot, bigger force needed
Static equilibrium
No movement
Often do not know the force at pivot point so torques=0
Clockwise torques=cc torques
Work
W=Fdcos(theta)
How much a force contributes to displacement
0<theta<90 Acting in x direction W is positive
theta=90 no force in same direction as d so W=0 because not helping d move
Bigger than 90 up to equal to 180 away from direction want to go taking away from direction d so W is negative
Work done be kinetic, centripetal, normal force
Kinetic: negative opposite of velocity
Centripetal: zero because always perpin. to motion
Normal: Usually zero perp. to motion but not if moving up and down
Work done by gravity
Wg=mgh
Gravity is a conservative force only depends on height
Power
P=W/t
depends on time now. So smaller time means more power
Also P=FV for constant force parallel to constant velocity
Kinetic energy
KE=1/2mv²
Total work W=deltaKE
Potential energy
Wgrav=-deltaPEgrav
deltaPEgrav=mgdeltaH
Systems
KE and PE convert into one another transforming but delta E=0
Spontaneous change/action always INCREASE in KE
Work can transfer energy into/out of a system
W done BY system Etotal is negative
W done ON system Etotal is positive
Conservation of energy equation
KEi+PEi=KEf+PEf
DeltaKE+deltaPE=0
Non conservative forces conservation of energy equation
KEi+PEi+Wnc=KEf+PEf
Wnc could be friction or tension for example
Inclined planes
Flipped so X component is mgsin(theta) and y is mgcos(theta)
Mechanical advantage
Fresistance or load/Feffort
Pullies provide multiples of force so MA of 4 is nice
Efficiency of energy
Woutput/Winput x 100%
Area under the curve
Calculate area under curve when the two variables are y and x
W=Fd
and F on y axis and d on x axis