1 00:00:00,950 --> 00:00:04,460 This week, we will continue our discussion of energy. 2 00:00:04,460 --> 00:00:07,020 We will introduce the concept of potential energy-- 3 00:00:07,020 --> 00:00:10,160 which is related to the work done by a conservative force, 4 00:00:10,160 --> 00:00:12,807 and also the concept of total mechanical energy-- 5 00:00:12,807 --> 00:00:15,140 which is defined as the sum of the kinetic and potential 6 00:00:15,140 --> 00:00:16,520 energies. 7 00:00:16,520 --> 00:00:19,070 We will demonstrate that the total mechanical energy 8 00:00:19,070 --> 00:00:22,310 of a system remains constant if only conservative forces are 9 00:00:22,310 --> 00:00:23,334 acting. 10 00:00:23,334 --> 00:00:25,250 This is known as the Principle of Conservation 11 00:00:25,250 --> 00:00:27,020 of Mechanical Energy. 12 00:00:27,020 --> 00:00:28,640 We will also see how the work done 13 00:00:28,640 --> 00:00:31,220 by any non-conservative forces causes 14 00:00:31,220 --> 00:00:33,140 the total mechanical energy of the system 15 00:00:33,140 --> 00:00:36,080 to change, usually causing mechanical energy to be 16 00:00:36,080 --> 00:00:38,430 lost from the system. 17 00:00:38,430 --> 00:00:41,600 Finally, we will see how graphs of a system's potential energy, 18 00:00:41,600 --> 00:00:43,760 as a function of position, provide 19 00:00:43,760 --> 00:00:46,040 an elegant way of understanding the behavior 20 00:00:46,040 --> 00:00:50,018 of the system for a given value of the total mechanical energy.