Steven W. answered 11/14/16
Tutor
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Physics Ph.D., college instructor (calc- and algebra-based)
Hi Lauren:
The work-(kinetic energy theorem can also be used here. See your previous post for my description of the theorem.
Making the same assumption Frank mentioned, that only friction is acting along the line of displacement, the work-(kinetic) energy theorem gives:
Wnet = Wf = KEf - KEi
Wf = Ffdcosα
Since friction always opposes any motion that is happening, it always points directly opposite displacement, and therefore, the angle between force and displacement is always 180o. So friction ALWAYS does negative work (cos(180o) = -1).
Wf = -Ffd
Ff = μkN
where N = normal force. On a horizontal surface, as described, where only the normal force and gravity act vertically, they must equal each other (since the net vertical acceleration is 0). So, N = mg, and
Ff = μkmg = (0.13)(40 kg)(9.8 m/s2) = 51 N
Then:
Wf = -Ffd = -(51 N)(11.4 m) = -581 J = KEf - KEi
We are told KEi = 2801 J. So we have:
-581 J = KEf - 2801 J
KEf = -581 + 2801 = 2220 J
I hope this helps! Just let me know if you have any questions about this.