If we ignore air resistance, then the range R(šœƒ) of a baseball hit at an angle šœƒ with respect to the x axis and with initial velocity v0 is given by

R(šœƒ) = 1/g(v0)2 sin (2šœƒ) for 0 ā‰¤ šœƒ < šœ‹/2

where g is the acceleration due to gravity.

(a) If v0 = 80 (meters per second) and g = 9.8 (meters per second per second), then

R ' (šœ‹/4)

a little more ligibly,

R = v^2/g sin2Īø

when you say R', derivative with respect to what?
Hmmm. it appears you mean dR/dĪø, with v constant.
dR/dĪø = 4v^2/g cos2Īø = 4*6400/9.81 * 1/āˆš2 = 1845.25 m/rad

R ' (šœ‹/4) is the derivative of the range function with respect to šœƒ, evaluated at šœ‹/4.

To find the derivative of R(šœƒ), we can apply the chain rule. The derivative of the outer function, sin(2šœƒ), is cos(2šœƒ). The derivative of the inner function, 2šœƒ, is simply 2. So, we have:

R ' (šœƒ) = 1/g(v0)^2 * cos(2šœƒ) * 2

Now, let's evaluate it at šœ‹/4:

R ' (šœ‹/4) = 1/g(v0)^2 * cos(2(šœ‹/4)) * 2

Since cos(2šœ‹/4) = cos(šœ‹/2) = 0, we have:

R ' (šœ‹/4) = 1/g(v0)^2 * 0 * 2

Simplifying further:

R ' (šœ‹/4) = 0

So, the derivative of the range function at šœ‹/4 is 0. It means that at an angle of šœ‹/4, the trajectory of the baseball is neither increasing nor decreasing in range. Perhaps the baseball is just enjoying the view from that angle, like a squirrel sitting on a branch, contemplating life before deciding to continue its journey.