 Ch 3. Particle Energy Methods Multimedia Engineering Dynamics Work &Energy Conservative Forces Power & Efficiency
 Chapter - Particle - 1. General Motion 2. Force & Accel. 3. Energy 4. Momentum - Rigid Body - 5. General Motion 6. Force & Accel. 7. Energy 8. Momentum 9. 3-D Motion 10. Vibrations Appendix Basic Math Units Basic Equations Sections Search eBooks Dynamics Statics Mechanics Fluids Thermodynamics Math Author(s): Kurt Gramoll ©Kurt Gramoll DYNAMICS - THEORY

Conservation of Energy Conservation of Energy for a
Spring-Mass System

In the previous section, Work and Energy was developed for a non-conservative system. However, in many problems there are only conservative forces which permits an alternative way to develop the energy balance equation.

A conservative force means that the work done by the force is independent of the path. Gravity and springs are conservative forces, but friction is not.

If there are only conservative forces, then the total energy at any point in time (or position) must be constant. Generally, conservative forces are grouped as potential (V) or kinetic (T) energy.

V1 + T1 = constant

If the total energy is constant, then the total energy at one point must equal the total energy at another point in the motion.

 V1 + T1 = V2 + T2

At any given time, all energy in a conservative system is defined as kinetic or potential energy. Kinetic Energy and Velocity

Kinetic (motion) Energy

Kinetic energy is based on the velocity of the object. Recall from the previous section,

T = ½mv2

Potential (stored) Energy Potential Energy

Energy that can be stored and converted to kinetic energy is referred to as potential energy,

Gravity Potential   Vg = mgy

Spring Potential     Vs = ½ks2

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