The figure below is a long stick with evenly spaced marks.The distance between two adjacent marks is 13.90 cm.
For each of the following forces or set of forces determine the
requested torque. Use Point L as the axis of rotation. Use the sign
convention that a counterclockwise (CCW) torque is considered
positive and a clockwise (CW) torque is considered
negative.
A force of 18.0 N is directed upward perpendicular to the stick at
Point G. What is the torque from this force?
A force of 29.0 N is directed downward perpendicular to the stick
at Point G. What is the torque from this force?
A force of 12.0 N is directed upward perpendicular to the stick at
Point C. What is the torque from this force?
A force of 28.0 N is directed upward at angle 32.1
Torque T=r*F sin(theta).....
A)T=5*13.9-69.5 cm...
F=18 N.....stick moves in CCW.....
T=12.51 N.m.......
B)T=.695 *29=-20.155 N.m....
riotates in CW....
C)T=3*0.139*12 =-5.004 N.m...rotates in CW..
D)T=5*0.139*28*sin(90-32.1)= -16.48 N.m
rotates in CW
E)T=0...since angle theta =0..hence
sin?=0....
F) Tnet =12.51-5.004 = 7.506 N.m
Use the formula T = r X F = |r||F| sin(\theta) , |r| is the
magnitude of the moment arm of the force from point G, |F| is the
magnitude of the force, and \theta is the angle (clockwise
positive) between the moment arm and the force
i) T = |r||F| sin(\theta) = 5d . 18 sin (90) = 12.51 Nm (using right hand rule)
ii) T = |r||F| sin(\theta) = 5d . 29 sin(-90) = -20.155 Nm
iii) T = |r||F| sin(\theta) = 3d . 12 sin(-90) = -5.004 Nm
iv) T = |r||F| sin(\theta) = 5d . 28 sin(90-32.1) = 16.485
v) T = |r||F| sin(\theta) = 5d . 29 sin(0) = 0
vi) T = sum( |r||F| sin(\theta)) = 5d . 18 sin(90) + 3d . 12
sin(-90)= 7.506
The figure below is a long stick with evenly spaced marks.The distance between two adjacent marks is 13.90 cm.
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To understand the two most
common procedures for finding torques when the forces and
displacements are all in one plane: the moment arm method and the
tangential force method. The purpose of this problem is to give you
further practice finding torques in two-dimensional situations. In
this case it is overkill to use the full cross product definition
of the torque because the only nonzero component of the torque is
the component perpendicular to the plane containing the problem.
There...