a) The work done by the horizontal force, F along the inclined plane is given by the dot product of that force vector and the distance vector traveled by the block, d. Since these vectors are parrel, The work done by the external force = Fd.
b) Taking the sum of differential work done by friction on the block across a distance, d, we have:
W = ∫0d Ff •dx = ∫0d Ff cos(180°)dx = ∫0d Ff (-1)dx = −∫0d Ff dx
where Ff is the force of friction as function distance = µFn = (bx)(mg cos(θ)),
where Fn = (mg cos(θ) is the normal force of the block. If confused about this value lookup "inclined block problem" so that you can see a diagram, there are many examples.
Finally, we have:
W = −∫0d Ff dx = −∫0d (bx)(mg cos(θ)) dx = −(bmg)(cos(θ)) ∫0d x dx = −(bmg)(cos(θ)) ( (1⁄2)x2 |d0 )
= −(bmg)(cos(θ)) ( (1⁄2)(d)2 − (1⁄2)(0)2) = −((1⁄2)bmgd2)(cos(θ))

Luke J.
That answers a & b, but where is part c?01/03/21