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Complicated collisions: the ballistic pendulum (I)

In real life, collisions are often messy affairs which require a mixture of techniques to understand. As an example, consider the ballistic pendulum.

You can break the action into two pieces:

  1. A ball of mass m moving at speed v1 slams into an arm of mass M. Use conservation of momentum in this completely inelastic collision to write an equation relating v1 to the velocity of the arm-plus-ball v2.
  2. An arm with an initial speed swings up until it halts at an angle theta. Use conservation of energy to figure out the relationship between the speed of the arm-plus-ball v2, the angle theta, and the height h by which the center of mass of arm-plus-ball rises.

Your first job today is to figure out the speed v1 with which the ball is fired from the catapult, by measuring the angle theta (and some other quantities).

You should end up with one table showing all your measurements, and the uncertainty associated with each measurement. You should also have a value of v1, the velocity of the ball when it leaves the muzzle of the gun.

Bonus! Compute the uncertainty in v1.


As you try to convert the uncertainties in the values you measured in class into an uncertainty in the initial speed v1 of the ball, you may find it useful to peruse


Your second job is to calculate the spring constant k of the spring in the gun.

Energy-based measurement
Use your measurements of the initial speed of the ball to compute the kinetic energy of the ball. Assume that this kinetic energy (KE) is exactly the same as the spring potential energy (SPE) stored in the compressed spring. Measure the distance -- and uncertainty -- by which the spring is compressed. Compute the spring constant.

Bonus: Compute the uncertainty in your value of the spring constant, using uncertainty in KE and uncertainty in distance compressed.


Creative Commons License Copyright © Michael Richmond. This work is licensed under a Creative Commons License.