A hanging spring is compressed 3 inches from its rest position and released at t = 0 seconds. It returns to the same position after 0.8 seconds.

what is the displacement from the rest position at t= 3 min rounded to the tenths place

What is the function that models the displacement, y, of the end of the spring from the rest position of time, t.

To find the displacement from the rest position at t = 3 min, we need to convert the time to seconds.

1 min = 60 seconds,
so 3 min = 3 * 60 = 180 seconds.

Given that the spring returns to the same position after 0.8 seconds, we can assume that it oscillates with a period of 0.8 seconds.

The general equation for the displacement of a spring undergoing simple harmonic motion is given by:

y(t) = A * cos(2π * f * t + φ),

where A is the amplitude (the maximum displacement from the rest position), f is the frequency (the number of oscillations per second), t is the time, and φ is the phase constant.

Since the spring is compressed 3 inches from its rest position, the amplitude A = 3 inches.

The frequency, f, can be determined using the equation f = 1 / T, where T is the period.

Given that the period T = 0.8 seconds, we have:

f = 1 / 0.8 = 1.25 Hz.

Now we can write the function for the displacement, y(t):

y(t) = 3 * cos(2π * 1.25 * t + φ).

To determine the phase constant φ, we can use the fact that the spring is released at t = 0 seconds and returns to the same position. This means that the initial phase is 0 radians.

Therefore, the function that models the displacement, y, of the end of the spring from the rest position as a function of time, t, is:

y(t) = 3 * cos(2π * 1.25 * t).

To find the displacement from the rest position of the hanging spring at t = 3 min, we can first convert the time from minutes to seconds. There are 60 seconds in a minute, so 3 minutes is equal to 3 * 60 = 180 seconds.

We are given that the hanging spring returns to the same position after 0.8 seconds. This means that the time it takes for the spring to complete one full oscillation is 0.8 seconds.

We can use this information to find the number of complete oscillations that occur in 180 seconds. Divide 180 seconds by 0.8 seconds to get:

Number of oscillations = 180 seconds / 0.8 seconds = 225 oscillations

Since the spring returns to the same position after each complete oscillation, we know that it will also be at the same position after 225 oscillations.

Next, we need to determine the displacement of the spring at the same position it started from, which is 3 inches from its rest position. We have to consider the fact that the displacement changes with each oscillation.

If the spring returns to the same position after each oscillation, it means that the displacement after an odd number of oscillations will be equal to the initial displacement (3 inches), while the displacement after an even number of oscillations will be in the opposite direction from the initial displacement.

In this case, since the number of oscillations is 225 (an odd number), the displacement at t = 3 min will still be 3 inches from the rest position.

Therefore, the displacement from the rest position at t = 3 min is 3 inches.

As for the function that models the displacement of the end of the spring from the rest position over time, it would depend on the specific characteristics of the spring and how it behaves. There are various mathematical models for spring motion, such as simple harmonic motion, damped harmonic motion, or forced harmonic motion, which may include constants and coefficients depending on the system. Without more specific information, it is difficult to provide an exact function that models the displacement.