A block attached to a spring is displaced from equilibrium to the position x=+0.5m and released. The period is 2.1s . At what positions and times during the first complete cycle do the following conditions occur.

a) |v|=0.5vmax, Where vmax is the maximum speed?

First position:
First time:

Second position:
Second time:

Third position:
Third time:

Fourth position:
Fourth time:

b) |a|=0.5amax, Where amax is the maximum magnitude of the acceleration?

First position:
First time:

Second position:
Second time:

Third position:
Third time:

Fourth position:
Fourth time:

Position in m and time in s pleaseeeee

To solve this problem, we need to use the equations for simple harmonic motion. In these equations, the position (x), velocity (v), and acceleration (a) of the block are related to time (t) and other parameters, such as the amplitude and period of the motion.

Given that the period of the motion is 2.1s, we can find the angular frequency (ω) using the formula:

ω = (2π) / T

where T is the period. Substituting the given value, we get:

ω = (2 * 3.14) / 2.1
≈ 2.99 rad/s

Now, let's solve both parts of the question.

a) |v| = 0.5vmax, where vmax is the maximum speed:

The maximum speed (vmax) of a system in simple harmonic motion is given by the formula:

vmax = A * ω

where A is the amplitude of the motion. In this case, since the block is displaced by x = 0.5m, the amplitude (A) is 0.5m.

vmax = 0.5m * 2.99 rad/s
≈ 1.495 m/s

To determine the positions and times during the first complete cycle when |v| = 0.5vmax, we use the equation for velocity:

v = ±A * ω * cos(ω * t)

We set |v| equal to 0.5vmax and solve for t. Note that the ± sign accounts for the fact that velocity changes direction during the motion.

0.5 * 1.495 = 0.5 * 0.5 m * 2.99 rad/s * cos(2.99 rad/s * t)

Dividing both sides by 0.5 m * 0.5 rad/s * 2.99 rad/s:

cos(2.99 rad/s * t) = 0.5

Using an inverse cosine function, we find:

2.99 rad/s * t = ±0.5236 rad

Simplifying:

t = ±0.5236 rad / 2.99 rad/s

≈ ±0.175 s

Since we need to consider both positive and negative times, we get the following positions and times during the first complete cycle:

First position: x = 0.5m, t = ±0.175s

Second position: x = 0m (equilibrium position), t = ±0.525s

Third position: x = -0.5m, t = ±0.875s

Fourth position: x = 0m (equilibrium position), t = ±1.225s

b) |a| = 0.5amax, where amax is the maximum magnitude of the acceleration:

The maximum magnitude of acceleration (amax) in simple harmonic motion is given by the formula:

amax = A * ω^2

Substituting the known values:

amax = 0.5m * (2.99 rad/s)^2
≈ 2.242 m/s²

To determine the positions and times during the first complete cycle when |a| = 0.5amax, we use the equation for acceleration:

a = -A * ω^2 * sin(ω * t)

We set |a| equal to 0.5amax and solve for t.

0.5 * 2.242 = -0.5 * 0.5 m * (2.99 rad/s)^2 * sin(2.99 rad/s * t)

Dividing both sides by 0.5 m * (2.99 rad/s)^2 * 0.5:

sin(2.99 rad/s * t) = -0.5

Using an inverse sine function, we find:

2.99 rad/s * t = -0.524 rad

t = -0.524 rad / 2.99 rad/s

≈ -0.175 s

Since acceleration changes direction during the motion, the negative time represents the same position as the positive time. Therefore, the positions and times during the first complete cycle are as follows:

First position: x = 0.5m, t = -0.175s

Second position: x = 0m (equilibrium position), t = 0s

Third position: x = -0.5m, t = -0.175s (same position as first position)

Fourth position: x = 0m (equilibrium position), t = 0s (same position as second position)

Note: The times provided are for one complete cycle. To find the specific times within the cycle for each condition, you can multiply these times by the number of cycles completed before the given condition is met.

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