For a projectile with linear drag, the vertical component of the position looks like:
\[y(t) = \frac{m}{b}\Big(v_{y,0} + \frac{mg}{b} \Big)\Big(1-e^{-bt/m}\Big) - \Big(\frac{mg}{b}\Big)t + y_0 \]
Approximate with a Power Series: Do a power series expansion of the vertical component of the position to third order with respect to the constant \(b\).
(modified from Taylor 2.25)
Consider a cyclist moving in a straight line and coasting to a stop under the influence of a quadratic air resistance \(\vec{F}_{drag}=-cv^2 \hat{v}\).
Anticipate the functional behavior: Before doing any calculation, sketch (by hand) what you expect the velocity vs time and the position vs. time graph to look like. Label interesting regions or points.
Calculate: Starting with Newton's 2nd Law, find the velocity and position of the cyclist as a function of time.
Dimensions: Check the dimensions of the answers.
(modified from Taylor 2.35)
Consider an object dropped near the surface of Earth and subject to a quadratic drag force from the air.
Anticipate the functional behavior: Before doing any calculation, sketch (by hand) what you expect the velocity vs time and the position vs. time graph to look like. Label interesting regions or points.
Calculate: Find the velocity as a function of time (the equation is in the textbook but I want to see the details of the calculations). Be sure to do any integrals involved.
Examine the Behavior of Functions: Plot the velocity and explain the features of this plot. Compare your plot to your hand-sketch and comment on similarities and differences.
Calculate: Find the position as a function of time (again, the equation is in the textbook but I want to see the details of the calculation). Be sure to do any integrals involved.