The aim of this experiment is to obtain the efficiency of a supplied catapult.

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Coursework Part 2        William Foley

Aim:

The aim of this experiment is to obtain the efficiency of a supplied catapult.

Introduction:

A catapult is the name given to any object that uses the principle of tension or sometimes torsion in order to discharge a smaller object and project it over a certain distance. There are many different types of catapults, for example the various engines of war used in ancient and medieval times to discharge javelins, darts, rocks, and other missiles; and also the forked objects with elastic attached to either branch which propels stones by using the principles of elastic potential energy. However, the catapult I will be testing will consist of a single piece of elastic attached between two stands, which will be clamped securely to a bench which will provide a sturdy base on which the catapult will fire.

  The aim of my experiment is to obtain the efficiency of a supplied catapult. I know from previous experiments that the efficiency of any energy transfer is defined as

Efficiency = Energy usefully transferred 

                        Total energy transferred

Efficiency is often expressed as a percentage. For example, consider a rower whose muscles are 20% efficient, then 20% of the energy transferred is useful and works the oars, however the remaining 80% is wasted due to temperature increase during exercise. I will therefore be presenting the value obtained of the efficiency of the catapult as a percentage.

  If I consider the equation above and relate it to the situation of investigating the efficiency of a catapult, I must first deduce how a catapult actually functions. Although certain catapults work in different ways, the catapult I am investigating works on the principle of converting elastic potential energy into kinetic energy in order to propel an object. This is achieved by the user pulling back on the elastic in order to increase the amount of tension in it. By performing this, elastic potential energy is induced into the elastic. When the user releases the elastic the elastic potential energy is then converted into kinetic energy which is provided to the object being projected. I can therefore consider that the type energy input is elastic potential energy and the energy output is kinetic energy. By inducing these factors into the equation I get

Efficiency =       Kinetic energy transferred

                     Elastic potential energy transferred

This is the equation I must consider in planning my experiment which means that I have to measure both the elastic potential energy obtained and the kinetic energy produced by the catapult when projecting an object.

  I am aware that Hooke’s law states that the extension or compression of an object is proportional to the force applied provided that the elastic limit is not reached. If the elastic used in my catapult, or any material in fact, obeys Hooke’s law it can be displayed on the following force-extension graph,

From this I can obtain a value for  elastic potential energy. The formula which can be used to find the elastic energy is:

Elastic energy = ½Fx

where ‘F’ is a force needed to produced an extension ‘x’.

By conducting a small experiment on the elastic used in my catapult in which I will measure values of force against extension, I will be able to plot a graph and calculate the area underneath in order to obtain a value that will represent the elastic energy in the material. This will provide me with a value which I can then substitute into my equation for obtaining the efficiency of the catapult as it represents ‘elastic energy transferred’ which is the ‘total energy transferred’ in the original equation.

  The process of obtaining a value for kinetic energy is a more difficult and more time consuming procedure. From earlier work I am familiar with the equation used for obtaining kinetic energy:

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Kinetic energy = ½ mv2

In the equation ‘m’ represents mass and ‘v’ represents velocity. The mass of the object will be easy to obtain however, the velocity in which the object travels will be difficult without the aid of expensive equipment. I will have to take into consideration the idea of projectile motion.

 In projectile motion, the displacement, velocity and acceleration of the projectile, in my case the ball bearing, are all vectors. The horizontal components can be treated as separate to the vertical components. If the ball laves the catapult horizontally, the initial velocity vector has ...

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