The vertical position of a ball suspended by a rubber band is given by the equation

y(t) = (3.4 m)sin(0.49 t/s − 0.40) − (0.4 m/s)t + 5.4 m.

(a) What are the equations for velocity and acceleration for this ball? (Use the following as necessary: t.)

(b) For what times between 0 and 30 s is the acceleration zero? (Enter your answers as a comma-separated list.)

(a) Well, let's do some math acrobatics here! To find the velocity function, we need to take the derivative of the position function, y(t). And when I say derivative, I'm not talking about a creepy dating app for mathematicians! So, grab your calculators and let's get derivative!

The derivative of sin(t) is cos(t), and the derivative of t is 1. So, the velocity function, v(t), is

v(t) = (3.4 m)cos(0.49 t/s − 0.40) − (0.4 m/s).

Now, for the acceleration function, we gotta get derivative-happy once again! Taking the derivative of cos(t) gives us -sin(t). So, the acceleration function, a(t), is

a(t) = -(3.4 m)sin(0.49 t/s − 0.40).

(b) Alrighty, let's find when the acceleration is zero between 0 and 30 seconds! Remember, we don't want any zeroes trying to crash the acceleration party! So, we set a(t) equal to zero and solve for t:

-(3.4 m)sin(0.49 t/s − 0.40) = 0.

Now, for sin(t) to be zero, t must be an integer multiple of π. So, we have:

0.49 t/s - 0.40 = nπ, where n is an integer.

Solving for t:

0.49 t/s = nπ + 0.40,

t = (nπ + 0.40) / 0.49.

Now, let's find the values of t between 0 and 30 seconds that satisfy this equation. Just plug in different integers for n and check for values within the given bounds. Be careful, this is not a clowning matter!

To determine the equations for velocity and acceleration, we need to take the derivatives of the position equation with respect to time.

(a) Velocity equation:
The derivative of the position equation, y(t), with respect to time, t, gives us the equation for velocity, v(t). So, let's calculate the derivative:

y(t) = (3.4 m)sin(0.49 t/s − 0.40) − (0.4 m/s)t + 5.4 m

dy/dt = d/dt [ (3.4 m)sin(0.49 t/s − 0.40) − (0.4 m/s)t + 5.4 m ]

To differentiate the terms separately:
d/dt [ (3.4 m)sin(0.49 t/s − 0.40) ] = (3.4 m) * d/dt [sin(0.49 t/s − 0.40)]
d/dt [ (0.4 m/s)t ] = (0.4 m/s) * d/dt[t] = 0.4 m/s
d/dt [ 5.4 m ] = 0

Using the chain rule, d/dt [sin(0.49 t/s − 0.40)] can be calculated:

d/dt [sin(u)] = cos(u) * d/dt[u]

Let u = 0.49 t/s − 0.40

d/dt [sin(0.49 t/s − 0.40)] = cos(0.49 t/s − 0.40) * d/dt[0.49 t/s − 0.40]
d/dt[0.49 t/s − 0.40] = 0.49/s * d/dt[t]

Substituting back into the equation:

dy/dt = (3.4 m) * cos(0.49 t/s − 0.40) * 0.49/s - 0.4 m/s

Thus, the equation for velocity, v(t), is:

v(t) = (3.4 m) * cos(0.49 t/s − 0.40) * 0.49/s - 0.4 m/s

Acceleration equation:
Now, we need to differentiate the velocity equation with respect to time to find the acceleration equation, a(t).

dv/dt = d/dt [(3.4 m) * cos(0.49 t/s − 0.40) * 0.49/s - 0.4 m/s]

Using the chain rule, we differentiate cos(0.49 t/s − 0.40):

d/dt [cos(u)] = -sin(u) * d/dt[u]

Let u = 0.49 t/s − 0.40

d/dt [cos(0.49 t/s − 0.40)] = -sin(0.49 t/s − 0.40) * d/dt[0.49 t/s − 0.40]
d/dt[0.49 t/s − 0.40] = 0.49/s * d/dt[t]

Substituting back into the equation:

dv/dt = (3.4 m) * (-sin(0.49 t/s − 0.40)) * 0.49/s

Simplifying further:

dv/dt = -1.6666 m/s^2 * sin(0.49 t/s − 0.40)

Thus, the equation for acceleration, a(t), is:

a(t) = -1.6666 m/s^2 * sin(0.49 t/s − 0.40)

(b) To find the times between 0 and 30 seconds where the acceleration is zero, we set the acceleration equation equal to zero and solve for t:

-1.6666 m/s^2 * sin(0.49 t/s − 0.40) = 0

sin(0.49 t/s − 0.40) = 0

To solve for t, we find the values of t that make sin(0.49 t/s − 0.40) equal to zero. These values correspond to the times when the acceleration is zero.

Sin(x) = 0 whenever x is an integral multiple of π (pi). Therefore, we need to solve:

0.49 t/s – 0.40 = nπ, where n is an integer.

Simplifying the equation, we solve for t:

0.49 t/s = nπ + 0.40

t = (nπ + 0.40) / 0.49

Now, we substitute different values for n (including negative and positive integers) in the equation to find the corresponding times t between 0 and 30 seconds when the acceleration is zero. We list all the values found, separated by commas.