Work-Energy theorem

Implications of the Arbitrarily Curtailed Electrodynamics Model 1. Particle Physics, Including Dipole Symmetry Some Overlooked Principles in Electrodynamics Work-Energy Theorem in a Replenishing Potential Environment The Extended Principles Permit COP >1.0 Electrical Power Systems Patenting and Discovery Activity Results of the Research Three Important Principles and Mechanisms... 

D. Work-Energy Theorem in a Replenishing Potential Environment... 

In the MEG, we do not destroy the potentializing source dipole, which is the magnetic dipole of the permanent magnet. We include the vacuum interaction with the system, and we also include the broken symmetry of the source dipole in that vacuum exchange—a broken symmetry proved and used in particle physics for nearly a half century, but still inexplicably neglected in the conventional Lorentz-regauged subset of the Maxwell-Heaviside model. We also use the extended work-energy theorem, as discussed. 

Using and applying the extended work-energy theorem for a replenishing potential environment... 

To explain this, we need to apply the Work-Energy theorem to this situation. Remember, the Work-Energy theorem is given by ... 

We can now substitute the Work-Energy theorem (assuming the mass remains constant in the volume element) ... 

For example, the work-energy theorem can be used to find the work done by expanding a gas in a piston (Figure 3.3). Suppose Pint > Pextl recalling the definition of pressure as force per unit area (P = F/A), this implies that there will be a net outward force on the piston. Work has to be done on the surrounding gas as the piston is moved outward from r = r to r = r2. 

Equation 3.12, the work-energy theorem, can be converted into a more convenient form for a gas in a piston in the geometry, as we showed in Equation 3.14 ... 

Relationship between the force and potential work-energy theorem). In order to establish a relationship between energy and work we shall consider a body in a stationary field. Acquire an elementary body s displacement dl. The internal forces of the field will produce the work dA equal to the potential energy change (dA= -dU). Therefore,... 

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