Mechanical Advantage of Pulleys, Study notes of Advanced Physics

Download Mechanical Advantage of Pulleys and more Study notes Advanced Physics in PDF only on Docsity! S2 - 1 Mechanical Advantage of Pulleys OBJECTIVE: The objective of this experiment is to study different pulley arrangements and determine their advantage and efficiency. THEORY: In general, people use machines to make work easier. Machines make tasks easier because they either decrease the force that the operator has to apply or because they increase the speed with which the task is performed. Essentially, a machine is any device used to change the magnitude or direction of a force. However, work or energy is never multiplied by a machine, i.e. “we can’t get something for nothing”. A simple machine is used to exert an output force (or torque) greater than the input force (or torque). The magnitude of the force multiplication is called the Mechanical Advantage. The Theoretical Mechanical Advantage or TMA for short, is simply the ratio of the output force (load) by the ideal input force (ideal effort): ideal iF F TMA 0= But in real situations frictional losses always occur. That is, the input force (real effort) is always greater than the effort that would be required in an ideal frictionless case. We define then the Actual Mechanical Advantage or AMA for short, as real iF F AMA 0= As far as work is concerned, in the ideal case, the input work equals the output work, i.e. i ideal i dFdF =00 (assuming, for simplicity, that in the definition of work the force and displacement have the same direction). Clearly, 0 0 d d F F TMA i ideal i == In the real case, the input work equals the output work plus lost energy. Thus, i ideal ifr dFdFW =+ 00 Where, Wfr is the work due to friction, the most common cause of energy loss. Machines and motors are quite common and we often talk about their efficiency. Simple or complex machines have mechanical parts that move, so some energy is always lost due to some friction or some other causes. That is, not all the input energy goes into doing work. Mechanical efficiency is essentially a measure of how much we get from the machine as compared to how much we put in. It is given as a percentage. For example, if a machine requires 100 J energy input and only produces 50 J of work we say that its efficiency is 50%. One can define efficiency, ε, in terms of work (W), energy (E) or power (P). Thus, the following definitions: TMA AMA P P E E W W in out in out in out ====ε S2 - 1 Note that in order to have an efficiency of 100% the AMA would have to equal the TMA. If 100% efficiency could be attained, a so-called perpetual motion machine could be devised. Using the machine’s output as input, would cause the machine to run for ever. Let’s now apply these concepts to pulley systems. Pulleys are said to be continuous levers. Figure 1 depicts a fixed (a) and a moving (b) pulley. Figure 1 – (a) Fixed and (b) Moving Pulley In a fixed pulley the TMA equals one. Assuming the pulley to be frictionless (ideal case) the tension throughout the rope is the same. That is, T1 = T2 and since the effort = T1 and load = T2 we immediately conclude that effort = load or ideal iFF =0 implying then that TMA = 1. In fact a fixed pulley only acts as a direction changer. On the other hand, for the moving pulley of figure 1 (b): Effort = T1 = T Load = T1 + T2 = 2T and clearly then TMA = 2. Of course, the input force will have to move twice as far as the load itself, moves. For example, to raise a load a distance of 1 metre, one would have to pull up a length of rope of two metres. In order to obtain a greater TMA one can use a system of several pulleys. There are several ways of arranging pulleys. Two particular types of pulley arrangements are known by the names of block and tackle. Using equilibrium conditions it is easy to determine the TMA of an arbitrary system of pulleys. Consider, for example, the system represented in Figure 2. Effort Load Effort Load T1 T2 T T T