An object with a mass of 5 kg5kg is pushed along a linear path with a kinetic friction coefficient of u_k(x)= x+xsinx uk(x)=x+xsinx. How much work would it take to move the object over x in [0, 8pi]x∈[0,8π], where x is in meters?
1 Answer
Explanation:
Work done by a variable force is defined as the area under the force vs. displacement curve. Therefore, it can be expressed as the integral of force:
color(darkblue)(W=int_(x_i)^(x_f)F_xdx)W=∫xfxiFxdx where
x_ixi is the object's initial position andx_fxf is the object's final position
Assuming dynamic equilibrium, where we are applying enough force to move the object but not enough to cause a net force and therefore not enough to cause an acceleration, our parallel forces can be summed as:
sumF_x=F_a-f_k=0∑Fx=Fa−fk=0
Therefore we have that
We also have a state of dynamic equilibrium between our perpendicular forces:
sumF_y=n-F_g=0∑Fy=n−Fg=0
=>n=mg⇒n=mg
We know that
vecf_k=mu_kmg→fk=μkmg
=>color(darkblue)(W=int_(x_i)^(x_f)mu_kmgdx)⇒W=∫xfxiμkmgdx
We have the following information:
|->"m"=5"kg"↦m=5kg |->mu_k(x)=x+xsin(x)↦μk(x)=x+xsin(x) |->x in[0,8pi]↦x∈[0,8π] |->g=9.81"m"//"s"^2↦g=9.81m/s2
Returning to our integration, know the
color(darkblue)(W=mgint_(x_i)^(x_f)mu_kdx)W=mg∫xfxiμkdx
Substituting in our known values:
=>W=(5)(9.81)int_(0)^(8pi)(x+xsinx)dx⇒W=(5)(9.81)∫8π0(x+xsinx)dx
Let's break the integral up using the sum rule.
The left is a basic integral, but the right will require integration by parts to solve.
" "u=x " " du=dx u=x du=dx
dv=sin(x)dx " " v=-cos(x)dv=sin(x)dx v=−cos(x)
We will have an integral of the form:
uv-vintduuv−v∫du
Therefore, for the right most integral, we obtain:
-xcos(x)-(int_(0)^(8pi)(-cos x)dx)−xcos(x)−(∫8π0(−cosx)dx)
=>-xcos(x)+int_(0)^(8pi)(cosx)dx⇒−xcos(x)+∫8π0(cosx)dx
We now have a basic integral.
Putting it all together:
(5)(9.81)[int_(0)^(8pi)(x)dx+{-xcos(x)+int_(0)^(8pi)(cosx)dx}](5)(9.81)[∫8π0(x)dx+{−xcos(x)+∫8π0(cosx)dx}]
Which we can now evaluate, yielding
Therefore, we have that the work done is