### Video Transcript

Two identical springs, each with
spring constant 20 newtons per meter, support a 15.0-newton weight as shown. What is the tension in spring
π΄? What is the amount of stretch of
spring π΄ from the rest position?

In this problem, weβll assume that
the springs are ideal, in other words, with a constant relationship between their
spring constant and their displacement, and weβll also assume that π, the
acceleration due to gravity, is exactly 9.8 meters per second squared.

Letβs start by highlighting some of
the critical information weβre given in this problem. First weβre told the spring
constant of each of the springs, 20 newtons per meter, and weβre also told that the
weight that these springs support is 15.0 newtons.

This is a two-part problem, where
in part one, weβre asked to solve for the tension in spring π΄; weβll call that
capital π sub π΄. And in part two of the problem, we
wanna solve for the amount of stretch that spring π΄ experiences from its initial
rest position; weβll call that Ξπ₯ sub π΄.

Now letβs begin on part one of this
problem, and weβll start by recalling what Hookeβs law states. Hookeβs law tells us that there is
a certain class of elastic materials or springs that obey this relationship.

The force πΉ used to stretch or
compress the spring is equal to the displacement of the spring from its equilibrium,
called π₯, multiplied by a constant, called π. In this problem, weβll assume that
the springs weβre working with are Hookean springs, meaning they obey Hookeβs
law.

With that as background, letβs draw
a free body diagram of our mass thatβs suspended by the springs. We have our mass, and gravity acts
down on it; weβll call that πΉ sub π. And then the spring forces due to
spring π΄ and spring π΅ act up and out on it at an angle of 30 degrees.

So the forces acting on our mass
are πΉ sub π, the force of gravity; π sub π΄, the tension in spring π΄; and π sub
π΅, the tension in spring π΅. And we know that because our mass
is not in motion, all these forces balance one another out. The acceleration of the mass is
zero.

To solve for π sub π΄, the tension
in spring π΄, which incidentally will be equal to ππ΅, letβs write a force balance
equation in the vertical direction based on Newtonβs second law.

As we use the second law to move
forward, letβs also define up as a direction of positive motion. We can now write out a vertical
force balance equation like this: the vertical component of π sub π΄, which is π
sub π΄ times the cosine of 30 degrees, plus the vertical component of π sub π΅, or
π sub π΅ times the cosine of 30 degrees, minus the force of gravity, which is the
mass of our block times π, is equal to zero.

And again thatβs true because our
block is not accelerating and so π in our second law is zero. Now as we look at this equation, we
can simplify it a bit based on the fact that our springs π΄ and π΅ are
identical. Therefore, we can write π sub π΅
as π sub π΄ because the springs are the same, which means we can simplify the
left-hand side of our equation to two times π sub π΄ cosine of 30 degrees.

We want to rearrange this equation
to solve for π sub π΄; thatβs what weβre looking for in part one of this
problem. To do that, we can add ππ to both
sides, which cancels out that term on the left-hand side of our equation. And we can then divide both sides
of the equation by two times the cosine of 30 degrees.

This results in the factors of two
and cosine of 30 canceling on the left-hand side of our equation, leaving us with π
sub π΄ by itself. Rewriting a simplified version of
this equation, we see that π sub π΄ is equal to ππ divided by two times the
cosine of 30 degrees.

Now interestingly, weβre not told
the mass π that is being suspended by the springs, but we are told that it has a
weight of 15.0 newtons. We can call that capital π. The weight is equal to the product
of the objectβs mass times the acceleration due to gravity. So in other words, we can replace
ππ in our equation for tension in spring π΄ with capital π, the weight.

We can now substitute in the given
value for π, 15.0 newtons, and enter this fraction on our calculator. This gives us a value for π sub π΄
of 8.7 newtons. Thatβs the tension in spring π΄, as
well as the tension in spring π΅ that is experienced when supporting this mass with
a weight of 15.0 newtons.

Now that we know π sub π΄, we can
move ahead with solving for Ξπ₯ sub π΄, the amount that spring π΄ is displaced from
equilibrium. To figure this out, we can refer
back to Hookeβs law.

We can apply Hookeβs law to our
scenario by restating it using our variables. Instead of πΉ equals negative ππ₯,
we can write π sub π΄ equals π times Ξπ₯ sub π΄. π sub π΄ is the tension in spring
π΄ we solved for in part one. π is the spring constant which
weβre given in the problem statement is 20 newtons per meter. And Ξπ₯ sub π΄ is the variable we
want to solve for, that is, the displacement from equilibrium that spring π΄
experiences under the stress of holding up the weight π.

So letβs rearrange this equation
for Ξπ₯ sub π΄ by dividing both sides by π, the spring constant. When we do that, π cancels out
from the right-hand side of our equation and weβre left with an equation that reads
Ξπ₯ sub π΄ is equal to π sub π΄ divided by π.

Plugging in for our given and
solved for values, we know π sub π΄ is 8.7 newtons and π is 20 newtons per
meter. Plugging these numbers into our
calculator, we find that Ξπ₯ sub π΄ is equal to 0.43 meters. Thatβs the distance from
equilibrium. That spring π΄ is stretched under
the weight of weight π.