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Presented by: Michael A Sierra, Jimmy Hernandez SC 441, Spring 2001, Professor Roman Kezerashvili Fgrav = m * g OBJECTIVES Determination of the kinetic and gravitational and potential energy of a body and an experimental test of the principle of conservation of mechanical energy in the gravitational field of the earth. Equipment Air track system with one glider. Science Workshop interface box. Two photogate accessories. Meter stick. Vernier caliper. Set of masses: 50 g and 100 g. Two blocks of cylinders. Theory There are two kinds of mechanical energy. The energy that an object possesses by virtue of its position, and is defined as potential energy. The gravitational potential energy is the energy that an object of mass m has by virtue of its position above the surface of the earth. In addition to having energy by virtue of its position, an object also possesses energy by virtue of its motion. The energy that an object possesses by virtue of its motion is the kinetic energy. The sum of these two kinds of energy are called the total mechanical energy E. E = U + K. In an isolated system, the total energy of the system remains a constant . This is the law (principle) of conservation of energy. In other words the principle of conservation of energy state that total mechanical energy remains a constant along all the path between the initial and final points, never varying from the initial value. The tendency of an object to conserve its mechanical energy is observed whenever external forces are not doing work. If the influence of friction and air resistance can be ignored (or assumed to be negligible) and all other external forces are absent or merely not doing work, then the object is often said to conserve its energy. “If only internal forces are doing work (no work done by external forces), there is no change in total mechanical energy; the total mechanical energy is said to be ‘conserved.’ ” Kinnetic energy gain, ∆K = ((mv22)/2) - ((mv21)/2) Loss in potential -∆U = -(mgy2 mgy1), J % difference 0.150 0.133 12.45 0.179 0.155 14.71 0.204 0.177 14.15 0.098 0.088 9.92 0.115 0.103 11.02 0.131 0.118 10.71 Table 2. Data and Results of Calculations Mass of Glider: .3Kg Height y1: .14m / .125m Length of Flag: .03m Height y2: .095m Position 1 Mass m, Kg Potential energy U1 = mgy1, J Position 2 Total energ y E1 = K1 + U1, J Velocit y V2 , m/ s Kinetic ene rgy k2 = mv2 2) / 2 Potentia l ene rgy E2 = K2 + U2, J Total ene rgy E2 = K2 + U2, J % Diff ere nce Velocity V1, m/s Kinetic energy k1 =(mv21)/2 0.301 0.485 0.035 0.412 0.448 1.111 0.185 0.280 0.465 3.85 0.351 0.482 0.041 0.481 0.522 1.120 0.220 0.326 0.546 4.60 0.401 0.481 0.046 0.549 0.596 1.117 0.250 0.373 0.623 4.42 0.301 0.394 0.023 0.368 0.391 0.897 0.121 0.280 0.401 2.33 0.351 0.394 0.027 0.429 0.457 0.901 0.142 0.326 0.469 2.60 0.401 0.392 0.031 0.491 0.521 0.899 0.162 0.373 0.535 2.52 Questions • Was the mechanical energy of the glider in motion conserved? Discuss the possible sources of error A/ Friction force from air Small friction force from air track system • A glider released from a starting height at an inclined air track bounces to one-half its original height. Discuss the energy transformations that take place. A/ In any isolated system, the total energy of the system remains constant along the paths between the initial and final points. Potential energy transforms to the kinetic energy of the glider and partially into internal energy of the glider (Heat energy ). In its simplest form, the ollie is a jumping technique that allows skaters to hop over obstacles and onto curbs, etc. What's so amazing about the ollie is the way the skateboard seems to stick to the skater's feet in midair. Seeing pictures of skaters performing soaring 4-foot ollies, many people assume that the board is somehow attached to the skater's feet. It's not. What's even more amazing about the ollie is that to get the skateboard to jump up, the skater pushes down on the board! The secret to this paradoxical maneuver is rotation around multiple axes. Let's take a closer look. Why are roller coaster loops made into egg-shaped ovals rather than circles? First, start with the fact that the ride begins by lifting the cars to a large height, then allowing gravity to power the rest of the ride. We can use conservation of energy and and knowledge of circular motion to predict what would happen for a circular loop as depicted below • We have proved the principle of conservation of mechanical energy, by calculating the gravitational potential energy which was found to be the same through out the experiment. The potential energy lost was equal to the kinetic energy gained. The total energy of the system was conserved. • One can use the transformation of energy in many cases, for example a ski jumper glides down the hill towards the jump ramp and off the jump ramp towards the ground. Potential energy is transformed into kinetic energy. Of course, it should be noted that the original assumption that was made for the ski jumper is that there were no external forces doing work. In actuality, there are external forces doing work.