A 3.60 kg object is attached to a vertical rod by two strings as in the figure below. The object rotates in a horizontal circle at constant speed 7.15 m/s.



(a) Find the tension in the upper string.
139 .
Your response is within 10% of the correct value. This may be due to roundoff error, or you could have a mistake in your calculation. Carry out all intermediate results to at least four-digit accuracy to minimize roundoff error. N

(b) Find the tension in the lower string.

To find the tension in the upper string, we can use the centripetal force equation:

F = mv^2 / r

where F is the centripetal force, m is the mass of the object, v is the velocity, and r is the radius of the circle.

Given:
m = 3.60 kg
v = 7.15 m/s

First, let's find the radius of the circle. Since the object is attached to a vertical rod, the tension in the lower string will act as the centripetal force, which means the tension in the lower string should be equal to the centripetal force:

F = T_lower

Next, let's find the tension in the lower string:

T_lower = mv^2 / r

Since the object is in a horizontal circle, the radius can be found using:

r = g / ω^2

where g is the acceleration due to gravity, and ω is the angular velocity.

Given:
g = 9.8 m/s^2

Now, let's find ω. The angular velocity can be found using the formula:

ω = v / r

Substituting the given values, we have:

ω = 7.15 m/s / r

Finally, we can substitute the value of ω into the equation for r:

r = g / ω^2
r = 9.8 m/s^2 / (7.15 m/s / r)^2
r = 9.8 m/s^2 / (51.1225 / r^2)
r = 9.8 m/s^2 * (r^2 / 51.1225)
r^3 = 5.2400518
r ≈ 1.81 m

Now, let's calculate the tension in the lower string:

T_lower = mv^2 / r
T_lower = 3.60 kg * (7.15 m/s)^2 / 1.81 m
T_lower ≈ 161.06 N

Therefore, the tension in the lower string is approximately 161.06 N.

To find the tension in the upper and lower strings, we can solve this problem using Newton's second law for circular motion.

(a) Finding the tension in the upper string:
In circular motion, there is a centripetal force that keeps the object moving in a circular path. This force is provided by the tension in the strings.

Let's analyze the forces acting on the object:
1. Tension in the upper string (T1), acting downwards.
2. Tension in the lower string (T2), acting upwards.
3. The weight of the object (mg), acting downwards.
4. The centripetal force (Fc), pointing towards the center of the circle.

Since the object is moving at a constant speed in a horizontal circle, the net force must be zero. Therefore, we can write the equation:

T1 - T2 - mg - Fc = 0

We know that Fc = (mv^2)/r, where m is the mass of the object, v is its speed, and r is the radius of the circle.
Let's denote the radius as "r".

The weight of the object is given by mg = 3.60 kg * 9.8 m/s^2 = 35.28 N.

Rearranging the equation, we get:
T1 - T2 = mg + Fc

Substituting the expression for Fc, we have:
T1 - T2 = 35.28 N + (3.60 kg * 7.15 m/s^2) / r

To find the tension in the upper string, T1, we need to solve for T1. Since the problem does not provide the radius of the circle, we cannot calculate the exact value of T1. Instead, we can determine the tension in the upper string as a function of the radius.

(b) Finding the tension in the lower string:
To find the tension in the lower string, T2, we can use the equation T1 - T2 = mg + Fc, which we derived in part (a).

Since we have already determined that T1 - T2 = 35.28 N + (3.60 kg * 7.15 m/s^2) / r, we can substitute the known values:

T1 - T2 = 35.28 N + (3.60 kg * 7.15 m/s^2) / r

To find T2, we need to find the value of T1 first. As mentioned before, we cannot calculate the exact value of T1 without knowing the radius.

Therefore, we are unable to determine the exact value of T2 without the radius of the circle.