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A part of the lecture notes for phys141, covering chapter 11 on torque and rotational motion. Topics include the definition of torque, the torque vector equation, net torque, torque and angular acceleration, work in rotational motion, power in rotational motion, and angular momentum. Important concepts such as the right-hand rule, the order of vector multiplication, and the relationship between torque and angular momentum are discussed.
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(vector product)
Depends on the choice of point O
The order in which the vectors are multiplied is important A x B = - B x A
If A is parallel to B (θ = 0 o^ or 180 o), then A x B = 0
d d d dt dt dt
A x (B + C) = A x B + A x C
m
r i j
F i j
= +
[(4.00^ ˆ 5.00 )N]ˆ^ [(2.00ˆ 3.00 )m]ˆ [(4.00)(2.00)ˆ ˆ^ (4.00)(3.00)ˆ^ ˆ (5.00)(2.00)ˆ ˆ^ (5.00)(3.00)ˆ^ ˆ 2.0 ˆN m
τ = × = + × + = × + ×
r F i j i j i i i j j i i j k
Two ways to understand torque equation:
(1) τ = F d
d: perpendicular distance from the axis of rotation to a line drawn along the direction of the force d = r sin Φ
(2) τ = Ft r F (^) t: tangential part of force F (^) t = F sin Φ
F 1 would cause counter- clockwise rotation about O F 2 would cause clockwise rotation about O
Total (net) torque = sum of torques
-> tangential acceleration:
Rotational motion description:
In general: Στ =Ια
2 t t t
Work done by F on the object as it rotates through an infinitesimal distance ds = r d θ dW = F.^ d s = ( F sin φ) r d θ