Example from Physics, 4.4 Newton's Third Law of Motion
A physics teacher pushes a cart of demonstration equipment to a classroom, as in Figure 4.11. Her mass is 65.0 kg, the cart’s mass is 12.0 kg, and the equipment’s mass is 7.0 kg. To push the cart forward, the teacher’s foot applies a force of 150 N in the opposite direction (backward) on the floor. Calculate the acceleration produced by the teacher. The force of friction, which opposes the motion, is 24.0 N.
Work it out on paper first. Then open the solution one step at a time, and stop as soon as you can finish on your own.
Because they accelerate together, we define the system to be the teacher, the cart, and the equipment. The teacher pushes backward with a force of 150 N. According to Newton’s third law, the floor exerts a forward force of 150 N on the system. Because all motion is horizontal, we can assume that no net force acts in the vertical direction, and the problem becomes one dimensional. As noted in the figure, the friction f opposes the motion and therefore acts opposite the direction of
We should not include the forces , , or because these are exerted by the system, not on the system. We find the net external force by adding together the external forces acting on the system (see the free-body diagram in the figure) and then use Newton’s second law to find the acceleration.
Newton’s second law is
The net external force on the system is the sum of the external forces: the force of the floor acting on the teacher, cart, and equipment (in the horizontal direction) and the force of friction. Because friction acts in the opposite direction, we assign it a negative value. Thus, for the net force, we obtain
The mass of the system is the sum of the mass of the teacher, cart, and equipment.
Insert these values of net F and m into Newton’s second law to obtain the acceleration of the system.
How did it go?