An object, previously at rest, slides 1 m1m down a ramp, with an incline of (3pi)/8 3π8, and then slides horizontally on the floor for another 2 m2m. If the ramp and floor are made of the same material, what is the material's kinetic friction coefficient?

1 Answer
Jul 23, 2017

mu_k = 0.388μk=0.388

Explanation:

WARNING: Long-ish answer

We're asked to find the coefficient of kinetic friction (mu_kμk) of an object sliding down a ramp.

![upload.wikimedia.org](useruploads.socratic.org)

We'll split this problem into two parts: the first part is where the object is sliding down the incline, and the second part is where it is sliding across the floor.

Incline:

The expression for the coefficient of kinetic friction mu_kμk is

f_k = mu_knfk=μkn

where

  • f_kfk is the magnitude of the retarding friction force acting as it slides down (denoted ff in the above image)

  • nn is the magnitude of the normal force exerted by the incline, equal to mgcosthetamgcosθ (denoted NN in the above image)

The expression for the net horizontal force sumF_(1x)F1x is

sumF_(1x) = overbrace(mgsintheta)^"gravitational force" - overbrace(f_k)^"kinetic friction force"

Since f_k = mu_kn, we have

sumF_(1x) = mgsintheta - mu_kn

And since the normal force n = mgcostheta,

sumF_(1x) = mgsintheta - mu_kmgcostheta

Using Newton's second law, we can find the expression for the acceleration a_(1x) of the object as it slides down the incline:

sumF_(1x) = ma_(1x)

a_(1x) = (sumF_(1x))/m = (mgsintheta - mu_kmgcostheta)/m = gsintheta - mu_kgcostheta

What we can now do is apply a kinematics equation for constant acceleration to find the final velocity v_(1x):

(v_(1x))^2 = (v_(0x))^2 + 2a_(1x)Deltax

Here, the initial velocity v_(0x) is 0, as we take it to start from rest (no value is given otherwise), and the distance Deltax it travels is the length of the incline (1 "m"), so we have

(v_(1x))^2 = (0)^2 + 2(gsintheta - mu_kgcostheta)(1color(white)(l)"m")

v_(1x) = sqrt(2(gsintheta - mu_kgcostheta)(1color(white)(l)"m"))

This velocity is also the initial velocity of the motion along the floor..

Floor:

As the object slides across the floor, the plane is perfectly horizontal, so the normal force n now equals mg. The only horizontal force acting on the object is the kinetic friction force f_k = mu_kn = mu_kmg (which is different than the first one).

The net horizontal force sumF_(2x) is thus

sumF_(2x) = overbrace(-f_k)^"negative because it opposes motion" = -mu_kmg

Using Newton's second law again, we can find the floor acceleration a_(2x):

a_(2x) = (sumF_(2x))/m = (-mu_kmg)/m = -gmu_k

We can now use the same constant-acceleration equation as before, but this time the initial velocity

v_(1x) = sqrt(2(gsintheta - mu_kgcostheta)(1color(white)(l)"m"))color(white)(aaa) (v_(1x) from above)

and the final velocity v_(2x) = 0 (it comes to rest).

Plugging in known values, we have

(0)^2 = (sqrt(2(gsintheta - mu_kgcostheta)(1color(white)(l)"m")))^2 + 2(-gmu_k)(2color(white)(l)"m")

Rearranging gives

2(gmu_k)(2color(white)(l)"m") = 2(gsintheta - mu_kgcostheta)(1color(white)(l)"m")

At this point, we're just solving for mu_k. Dividing both sides by 2g:

mu_k(2color(white)(l)"m") = (sintheta - mu_kcostheta)(1color(white)(l)"m")

Now, we can divide all terms by mu_k, as well as eliminate the unit "m":

2 = (sintheta)/(mu_k) - costheta

(sintheta)/(mu_k) = 2+costheta

Therefore,

color(red)(mu_k = (sintheta)/(2+costheta)

Plugging in the angle theta = (3pi)/8, we have

mu_k = (sin((3pi)/8))/(2+cos((3pi)/8)) = color(blue)(0.388

Notice how the coefficient doesn't depend on the mass m or gravitational acceleration g if the two surfaces are the same...