### Video Transcript

A box of mass 12.4 kilograms slides
from rest downward along a 1.58-meter-length ramp that is inclined at 23.3 degrees
below the horizontal. The coefficient of kinetic friction
between the box and the ramp is 0.0346. What is the magnitude of the boxβs
acceleration? What is the speed of the box at the
bottom of the ramp?

We can call the boxβs acceleration
π and the boxβs speed at the bottom of the ramp π£ sub π. Letβs start on our solution by
drawing a diagram of the moving box. In this example, we have a box of
mass π β π is 12.4 kilograms β on a ramp of length π, where π is 1.58
meters. The ramp is inclined at an angle
weβve called π, where π is 23.3 degrees above the horizontal. Under the influence of gravity, we
expect the box to slide down the ramp. and we want to solve for its acceleration,
π, when it does so. We also wanna find out how fast the
box is moving when it gets to the bottom of the ramp.

Into this scenario, we set up an
π₯- and a π¦-coordinate axis so that positive motion in the π₯-direction is down the
incline and positive motion in the π¦-direction is perpendicular to the plane. Next, letβs draw a free body
diagram of the mass π, that is, the forces that act on it. We know thereβs a gravitational
force acting on π straight down of magnitude π times π, where π, the
acceleration due to gravity, is 9.8 meters per second squared. Thereβs also a normal force acting
on the mass to keep it from moving into the plane. And lastly, as the box slides down
the plane, thereβs a kinetic frictional force that resists its motion.

Looking at this free body diagram,
we can divide up the weight force into its π¦- and π₯-components so that we can
write out force balance equations in the π¦- and π₯-directions. And we know that, with these force
components at a right angle to one another, a triangle is formed, where the upper
angle is the angle π.

Recalling Newtonβs second law of
motion, that the net force on an object equals its acceleration times its mass, we
can consider the forces in the π₯-direction in our scenario. Those are the kinetic friction
force and the π₯-component of the weight force. Since weβve decided that motion
down the ramp is motion in the positive direction, our force balance equation for
the π₯-forces is ππ sin π minus the kinetic friction force is equal to the mass
of the object times its acceleration.

The kinetic friction force, π sub
π, is equal to the coefficient of kinetic friction, π sub π, multiplied by the
normal force acting on an object. This means we can replace π sub π
with π sub π π sub π in our π₯-force balance equation. And we remember that weβre given π
sub π in the problem statement.

Looking at this force balance
equation, we see that if we divide both sides by the mass π, we see we have an
expression for the acceleration π we want to solve for. The one challenge is, we donβt yet
know the normal force, π sub π, that acts on our mass. To find that out, letβs look at the
forces in the π¦-direction on our mass.

Applying Newtonβs second law to
forces in this direction, we write that the normal force minus ππ cos π, the
π¦-component of the weight force, is equal to the mass of the box times its
acceleration in the π¦-direction. But because the box doesnβt leave
the surface of the plane, this acceleration is zero. And our equation simplifies to the
normal force is equal to ππ times the cos of π. This is perfect because now we can
take this term for π sub π and substitute it into our equation in the
π₯-direction.

With this expanded expression for
the acceleration π, we see that the boxβs mass π appears in all the terms in the
numerator and the denominator. So it cancels out. Factoring out the acceleration due
to gravity, π is equal to π times the quantity sin π minus π sub π cos π. Substituting in for π, π, and π
sub π, when we calculate π, to three significant figures, we find itβs 3.56 meters
per second squared. Thatβs the acceleration of the box
as it descends the ramp.

Next, we wanna solve for the speed
the box has when it reaches the bottom of the 1.58-meter-long ramp. To figure this out, we know that
the acceleration the box undergoes during its journey is constant. This means that the kinematic
equations of motion apply to the motion of this box. As we look over these four
equations of motion, we seek one that lets us solve for final velocity, π£ sub π,
in terms of information we know.

The second kinematic equation
written matches our conditions well. Rewriting it in terms of our
variables, the final speed of the box squared is equal to the boxβs initial speed,
which is zero because the box starts from rest, plus two times the boxβs
acceleration times the length of the ramp, π. If we take the square root of both
sides of this equation, we find that π£ sub π is equal to the square root of two
times π times π.

We know π from part one and π is
given information. So weβre ready to plug those in to
our expression. When we do, when enter these values
on our calculator, we find that π£ sub π is 3.36 meters per second. Thatβs the speed of the box when it
reaches the bottom of the ramp.