Hello mandy9008,
mandy9008 said:
if it is moving at a constant speed then the net work will be zero, right? I remember my professor saying that in class, but he never explained why.
Be careful how you interpret that, but yes, it is essentially true if you consider
all the relevant individual forces involved, even frictional forces if they apply (and they do in this problem), and potential energy related forces (which don't apply in this problem).
When contemplating the issue, ask yourself these questions:
(a) If an object is moving at a constant velocity, what does that tell you about its acceleration
a?
(b) Knowing that
Fnet =
ma, and if you also happen to know that
a = 0, what does that tell you about
Fnet (where
Fnet can be the sum of multiple forces)? Thus what can you conclude about all the individual forces that make up
Fnet? (Hint: if you were thinking that it means each of the individual forces making up
Fnet is zero, that's not generally true. But you can say something about how they combine together.)
(c) If an object does not change velocity, what does that tell you about the object's
change in kinetic energy?
(d) If an object's kinetic energy and potential energy do not change, what does that say about the total mechanical work done
on that object by the all forces acting
on that object?
I am guessing that there is some force that is equal and opposite of the work done by the shopper, which could be explained by Newton's third law
You're comparing work and force on equal terms. They are different things.
But you are on the right track. There must be some sort of force (or component of which that is doing work) that is equal in magnitude and opposite in direction to the component of the shopper's force that happens to be doing work.
To find out which forces do work and how much, find the
component of each force that is parallel to the displacement vector. (For example, if a force is completely perpendicular to the displacement, you can ignore it because it's not doing any work. If a force is at some sort of angle to the displacement vector, you need to find the component of that force which is parallel to the displacement vector to calculate how much work the force does.)