A uniform 1.3-kg rod that is 0.80 m long is suspended at rest from the ceiling by two springs, one at each end of the rod. Both springs hang straight down from the ceiling. The springs have identical lengths when they are unstretched. Their spring constants are 60 N/m and 35 N/m. Find the angle that the rod makes with the horizontal.

Assume g= 10 m/sec2

60*x1 + 35*x2 = 1.3*10=13

on observation we get
x1= 0.1 m
x2= 0.2 m

so tan(angle)= .1/.8= .125
angle= 7.125 degree

To find the angle that the rod makes with the horizontal, we can use the concept of equilibrium.

When the rod is at rest, the forces acting on it must balance out. These forces include the weight of the rod and the forces from the two springs.

Let's break down the problem into two parts, considering each spring and its force separately.

First, let's consider the left spring. The force from this spring can be represented as F1 = k1 * x1, where F1 is the force, k1 is the spring constant, and x1 is the displacement of the left end of the rod from its unstretched position.

Next, let's consider the right spring. The force from this spring can be represented as F2 = k2 * x2, where F2 is the force, k2 is the spring constant, and x2 is the displacement of the right end of the rod from its unstretched position.

Since the springs are identical in length when they are unstretched, the displacements x1 and x2 will be equal.

Now, let's consider the weight of the rod. The weight can be represented as W = m * g, where W is the weight of the rod, m is the mass of the rod, and g is the acceleration due to gravity (approximately 9.8 m/s^2).

In equilibrium, the forces from the two springs and the weight must balance out. Therefore, the vertical component of the forces from the two springs should add up to the weight of the rod.

The vertical component of the force from the left spring can be represented as F1y = F1 * sin(theta), where theta is the angle that the rod makes with the horizontal.

Similarly, the vertical component of the force from the right spring can be represented as F2y = F2 * sin(theta).

The weight of the rod can be represented as W = m * g.

Since we mentioned earlier that the vertical component of the forces from the two springs should add up to the weight of the rod, we can write the equation as:

F1y + F2y = W

Substituting the earlier equations, we have:

(k1 * x1 * sin(theta)) + (k2 * x2 * sin(theta)) = m * g

Next, let's substitute the values given in the problem.

m = 1.3 kg
k1 = 60 N/m
k2 = 35 N/m
g = 9.8 m/s^2

We need to determine the values of x1 and x2.

To find the displacements x1 and x2, we can use Hooke's law, which states that the force exerted by a spring is directly proportional to its displacement from its equilibrium (unstretched) position.

We can represent this as:

x1 = F1 / k1
x2 = F2 / k2

Substituting the given values, we have:

x1 = F1 / k1 = (m * g) / k1 = (1.3 kg * 9.8 m/s^2) / 60 N/m
x2 = F2 / k2 = (m * g) / k2 = (1.3 kg * 9.8 m/s^2) / 35 N/m

Once we determine x1 and x2, we can substitute these values back into the earlier equation:

(k1 * x1 * sin(theta)) + (k2 * x2 * sin(theta)) = m * g

Solving this equation for theta will give us the angle that the rod makes with the horizontal.