This example of torque
is a simple one because the force is in a plane perpindicular to the axis
of rotation. However, if you place unequal forces on a see-saw, it does not
always stay horizontal, as Johnny and Jane soon found out.
For the see-saw to stay horizontal, that is to stay in equilibrium,
the net torque would have to equal zero:
So how exactly
do we know which side of the see-saw will go up, and which side will go down?
To understand this, we can find the net torque of the see-saw.
First, we have to find the torque acting on each lever arm.
Johnny and Jane are sitting an equal distance of 1 meter from the axis of
rotation. Johnny has a mass of 20 kg, and Jane has a mass of 22 kg. The force
in this problem is the force the weight of an object on earth, or W=mg, where
m is mass and g is acceleration due to gravity (9.8m/s²).
Torque acting on Johnny's side of the see-saw:
T = Fl
T = (22 kg)(9.8 m/s²)(1 m)
T = 215.6 N*m
Torque acting on Jane's side
of the see-saw:
T = (20 kg)(9.8 m/s²)(-1 m)
T = -196 N*m
Net Torque acting on the see-saw:
215.6 N*m + -196 N*m
= 19.6 N*m