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Chapter 3 Kinetics of Particles 2142211 Dynamics, NAV 1 3-2 Work and Energy 2142211 Dynamics, NAV 2 3-2. Work and Energy 1. Work and Kinetic Energy Definition of Work Calculation of Work Work of Linear Spring Work and Curvilinear Motion Principle of Work and Kinetic Energy Advantage of Work-Energy Method Power Examples 2. Potential Energy Gravitational PE Elastic PE Examples Examples 2142211 Dynamics, NAV 3 3-2. Work and Energy 1. Introduction Recall Newton’s second law and notice that this is an instantaneous relationship. When we want to see changes in velocity or position due to motion, we have to integrate Newton’s second law by using appropriate kinematic equations. However, we may integrate Newton’s second law directly and avoid solving for acceleration first. In general, there is two classes of problems Integration with respect to displacement → Work-Energy equation → velocity between two positions of a particle or system’s configurations. Integration with respect to time → Impulse-Momentum equation → changes in velocity between two points in time. 2142211 Dynamics, NAV 4 3-2. Work and Energy 2. Definition of Work 2142211 Dynamics, NAV 5 3-2. Work and Energy 3. Calculation of Work 2142211 Dynamics, NAV 6 3-2. Work and Energy 3. Calculation of Work Notes: 2142211 Dynamics, NAV 7 3-2. Work and Energy 3. Calculation of Work Example 1: Collar and Guide Find the work done by the 8 N force on the collar when it moves from point A to point B. 2142211 Dynamics, NAV 8 3-2. Work and Energy 3. Calculation of Work Example 2: Collar and Guide Find the work done by the force F on the collar when it moves from point A to any point. 2142211 Dynamics, NAV 9 3-2. Work and Energy 3. Calculation of Work Example 2: continued 2142211 Dynamics, NAV 10 3-2. Work and Energy 4. Work of Linear Spring Linear spring F = kx where F is the force acting on the spring to compress/extend Work done on the spring by the body → use F Work done on the body by the spring → use P = -F Thus work done on the body by the spring is → → → → 2142211 Dynamics, NAV 11 3-2. Work and Energy 5. Work and Curvilinear Motion 2142211 Dynamics, NAV 12 3-2. Work and Energy 6. Work and Kinetic Energy 2142211 Dynamics, NAV 13 3-2. Work and Energy 6. Work and Kinetic Energy 2142211 Dynamics, NAV 14 3-2. Work and Energy 6. Work and Kinetic Energy Example 3: Collar and Guide again 2142211 Dynamics, NAV 15 3-2. Work and Energy 7. Power 2142211 Dynamics, NAV 16 3-2. Work and Energy 8. Potential Energy Gravitational PE Elastic PE 8.1 Gravitational PE (Vg) Reference 2142211 Dynamics, NAV 17 3-2. Work and Energy 8.1 Gravitational PE (Vg) Start low finish high = go up ΔVg = + Start high finish low = go down ΔVg = - 2142211 Dynamics, NAV 18 3-2. Work and Energy 8.2 Elastic PE (Ve) x is how much the spring is compressed or extended from its relaxed (original length) 2142211 Dynamics, NAV 19 3-2. Work and Energy 9. Alternate form of Work-KE equation 2142211 Dynamics, NAV 20 3-2. Work and Energy 9. Alternate form of Work-KE equation 2142211 Dynamics, NAV 21 3-2. Work and Energy 9. Alternate form of Work-KE equation 2142211 Dynamics, NAV 22 3-2. Work and Energy 9. Alternate form of Work-KE equation Special Case (when there is no work from the external force other than mg and spring) Law of Conservation of Mechanical Energy 2142211 Dynamics, NAV 23 3-2. Work and Energy Example 4: Slider Ans: 4.48 m/s 2142211 Dynamics, NAV 24 3-2. Work and Energy Example 5: Swinging Ball Ans: 3.59 m/s 2142211 Dynamics, NAV 25 3-2. Work and Energy Example 6: Spring and Slider Ans: 1.16 m/s 2142211 Dynamics, NAV 26 3-2. Work and Energy Example 7: Spring and Slider Ans: 3.59 m/s 2142211 Dynamics, NAV 27 3-2. Work and Energy Example 8: Slider The spring of stiffness k is compressed and released, sending the particle of mass m sliding along the track. Determine the minimum spring compression for which the particle will not lose contact with the track. The sliding surface is smooth except shown. 2142211 Dynamics, NAV 28