Projectile motion puzzle solution

This post captures my notes on the following problem from the last post:

Problem: Suppose that you are standing on the outer bank of a moat surrounding a castle, and you wish to secretly deliver a message, attached to a large rock, to your spy inside the castle.  A wall h=11 meters high surrounds the castle, which is in turn surrounded by the moat which is d=19 meters wide.  At what angle should you throw the rock in order to have the best chance of clearing the wall?

Solution: A projectile thrown from the origin with initial speed v at an angle \theta has a trajectory described by

x(t) = v t \cos \theta

y(t) = v t \sin \theta - \frac{1}{2} g t^2

Setting x(t)=d and y(t)=h and solving for v and t, we find the following expression for the required initial speed as a function of the throwing angle:

v(\theta)^2 = \frac{g d^2}{2 \cos^2 \theta (d \tan \theta - h)}

We can minimize this required initial speed by maximizing the denominator.  Differentiating and setting equal to zero yields

\tan 2\theta = -\frac{d}{h}

Keeping in mind that the throwing angle is between 0 and 90 degrees, we can rewrite this expression as

\theta = \frac{\phi + \pi/2}{2}

where \phi is the angle of the line of sight to the top of the wall.  The geometric interpretation of this result is: to have the best chance of clearing the wall, throw at an angle halfway between the line of sight to the top of the wall and the vertical.  In the original problem, this optimal throwing angle is about 60.03 degrees.

Recall, however, that this analysis assumes negligible effects of air resistance.  This is a safe assumption for a relatively heavy rock at human-throwable speeds, but not for a baseball.  If we apply this same analysis to Jackie Bradley, Jr.’s throw from home plate over the center field wall, 420 feet away and 17 feet high, we get an optimal throwing angle of about 46.2 degrees, with a minimum initial speed of only about 80.9 miles per hour, which is not terribly difficult to achieve.

To more accurately model the trajectory of a thrown (or batted) baseball, we must incorporate the effects of not only drag, which slows the ball down, but also the Magnus force, which “lifts” the ball causing it to “rise” and/or curve.  The references below describe several interesting experiments tracking thrown and hit baseballs, including some useful approximation formulas for accurately modeling these trajectories, yielding my estimate from the last post that Bradley must have thrown the ball at over 105 miles per hour, with an optimal throwing angle of just a little over 30 degrees.

Since this is the sort of problem that I think is excellent for students to attack via computer simulation, following are the relevant formulas and constants collected in one place for them to use:

The acceleration of a thrown or batted baseball due to gravity, drag, and lift is given by

a = g + a_D + a_L

a_D = -\frac{1}{2m}\rho v^2 A C_D \hat{v}

a_L = \frac{1}{2m}\rho v^2 A C_L (\hat{\omega} \times \hat{v})

where:

  • Acceleration due to gravity |g| = 9.80665 meters/second^2
  • Mass m = 5.125 ounces (the midpoint of the regulation tolerance)
  • Air density \rho = 1.225 kilograms/meter^3 (sea level on a standard day)
  • v and \omega are the magnitudes of velocity and angular velocity, respectively, with \hat{v} and \hat{\omega} being corresponding unit vectors in the same direction
  • A = \pi r^2 is the cross-sectional area of the baseball, where the circumference 2\pi r = 9.125 inches (the midpoint of the regulation tolerance)
  • Coefficient of drag C_D = 0.35 (see Reference 3)
  • Coefficient of lift C_L = S/(0.4+2.32S), where S = r\omega/v is the “spin parameter” (see Reference 2)
  • Backspin on a typical fastball \omega = 1500 rpm (or 2000 rpm for a typical batted ball; see Reference 1)

 

References:

1. A. Nathan, The effect of spin on the flight of a baseball, American Journal of Physics, 76:2 (February 2008), 119-124 [PDF]

2. A. Nathan, What New Technologies Are Teaching Us About the Game of Baseball, October 2012 [PDF]

3. D. Kagan and A. Nathan, Simplified Models for the Drag Coefficient of a Pitched Baseball, The Physics Teacher, 52 (May 2014), 278-280 [PDF]

 

This entry was posted in Uncategorized. Bookmark the permalink.

2 Responses to Projectile motion puzzle solution

  1. I put some time into encoding this into something that I can give to Octave’s lsode() ODE solver, but have so far been unsuccessful. Is this a reasonable approach?

    • Yes, I think so. I am not familiar with lsode(), but it looks like it’s similar to MATLAB’s ODE solvers, which would also work. (MATLAB’s also have “events” which can terminate integration early when specified conditions are satisfied, such as “the ball reaches the wall,” or “the ball hits the ground.” Octave may have something similar?)

      Note, however, that simple Euler integration will work just fine here as well, as long as your step size is small– I’m thinking like a teacher here, where (1) it’s much easier to explain v+=a*dt, and (2) if you’re actually animating/visualizing the entire trajectory, then you need a small step size anyway.

Leave a Reply

Fill in your details below or click an icon to log in:

WordPress.com Logo

You are commenting using your WordPress.com account. Log Out / Change )

Twitter picture

You are commenting using your Twitter account. Log Out / Change )

Facebook photo

You are commenting using your Facebook account. Log Out / Change )

Google+ photo

You are commenting using your Google+ account. Log Out / Change )

Connecting to %s