Henry P. answered 25d
5+ Years of Tutoring Physics
This is an example of a Conservation of Energy lab assignment.
When the bullet is sent flying with some initial horizontal velocity, it contains a certain amount of Kinetic Energy (the energy of any mass in motion) according to the formula KE = 1/2 m*v2
When the bullet strikes and is embedded in the ballistic pendulum, they combine and are treated as one mass. This is what we call a perfectly inelastic collision. An inelastic collision means that momentum is not conserved, but that's okay since momentum isn't what we're tracking in this lab. Energy of the bullet-pendulum system is conserved thanks to the Law of Conservation of Energy. Since the bullet and pendulum combined (m+M) have much greater mass than the bullet alone (m), we expect the velocity of the system to be proportionately smaller according to the formula
1/2 m*v12=1/2(m+M)*v22
As the pendulum swings upward, the initial kinetic energy of the system is changed into gravitational potential energy, the form of energy that object with mass acquire when they are moved up against the force of gravity. At the top of the pendulum's swing, all of the system's kinetic energy has been converted into gravitational potential energy. Since we can measure the change in elevation of the pendulum-bullet system (Δh), we can easily determine the final gravitational potential energy according to the formula
PE = (m+M)g*Δh
Since energy in this system is conserved (and there is no outside force acting to add or take away energy), we can set the final potential energy equal to the bullet's initial kinetic energy. As long as we know the mass of the bullet (m) and pendulum (M), the bullet-pendulum system's final height (Δh), and the acceleration due to gravity (g), we can solve for the bullet's initial velocity (vi) through the following equation:
1/2 m*vi2 = (m+M)g*Δh
vi2 = 2(m+M)g*Δh/m
vi = sqrt[2(m+M)g*Δh/m]
Differences between measured and theoretical answers to this problem may arise from energy loss due to air resistance on the bullet or friction in the pendulum, both of which represent not a violation of the Law of Conservation of Energy, but merely energy being transferred into less useful forms (airflow, heat) during the course of the experiment.