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Find when velocity is zero

A particle moves along a straight line with position function s(t)=5cos⁡(t)−ts(t) = 5\cos(t) - t, where tt is measured in seconds and ss in meters, for 0≤t≤2π0 \le t \le 2\pi.

Find all times tt in the interval [0,2π][0, 2\pi] at which the particle's velocity is zero.

Hint

Compute v(t)=s′(t)v(t) = s'(t), set it equal to zero, and solve for tt using the unit circle on the given interval.

Step-by-step solution

Differentiate s(t)=5cos⁡(t)−ts(t) = 5\cos(t) - t to get the velocity function: v(t)=s′(t)=−5sin⁡(t)−1v(t) = s'(t) = -5\sin(t) - 1.

Set v(t)=0v(t) = 0: −5sin⁡(t)−1=0-5\sin(t) - 1 = 0, so sin⁡(t)=−15\sin(t) = -\dfrac{1}{5}. On [0,2π][0, 2\pi], sine is negative in the third and fourth quadrants, giving t=π+arcsin⁡(1/5)≈3.3436t = \pi + \arcsin(1/5) \approx 3.3436 and t=2π−arcsin⁡(1/5)≈6.0812t = 2\pi - \arcsin(1/5) \approx 6.0812.

Classify motion at each critical time

At each time found in part (a), determine the direction of motion immediately after that instant. Use the sign of the acceleration to determine whether the particle begins moving forward or backward.

Hint

Find a(t)=v′(t)a(t) = v'(t), evaluate its sign at each critical time. Since v(t)=0v(t) = 0 at these times, the sign of a(t)a(t) determines the sign of vv immediately after, which tells you the direction of motion.

Step-by-step solution

Differentiate the velocity function to get acceleration: a(t)=v′(t)=−5cos⁡(t)a(t) = v'(t) = -5\cos(t). Evaluate cos⁡(t)\cos(t) at each critical time: at t=π+arcsin⁡(1/5)≈3.3436t = \pi + \arcsin(1/5) \approx 3.3436, tt is in the third quadrant so cos⁡(t)<0\cos(t) < 0, giving a(t)>0a(t) > 0; at t=2π−arcsin⁡(1/5)≈6.0812t = 2\pi - \arcsin(1/5) \approx 6.0812, tt is in the fourth quadrant so cos⁡(t)>0\cos(t) > 0, giving a(t)<0a(t) < 0.

At t≈3.3436t \approx 3.3436, we have v(t)=0v(t) = 0 and a(t)>0a(t) > 0. Since acceleration is positive, vv is increasing near this time, so vv transitions from negative to positive. Therefore, the particle begins moving in the forward (positive) direction immediately after this time.

At t≈6.0812t \approx 6.0812, we have v(t)=0v(t) = 0 and a(t)<0a(t) < 0. Since acceleration is negative, vv is decreasing near this time, so vv transitions from positive to negative. Therefore, the particle begins moving in the backward (negative) direction immediately after this time.

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