The term free energy potential energy has become an important tool for studying energy transitions in a wide variety of biological and chemical systems. The use of equation (11) for discussing the thermodynamic equivalency of kinetic energy and potential energy was first made widely known by the French physicist René Desmedt in the 18th century. It is derived using the principle of kinetic energy conversion, which was first defined by Le Quéré in 1761, and then subsequently elaborated by Joule and Laplace in 1848, 1859, and 1861 respectively.
Free Energy Potential Energy (free energy potential energy, FEPE)
This term is used to define the energy of a system in terms of an equilibrium that is assumed to exist in that system. If the system is in equilibrium, then the FEPE is zero. This is because each particle of a system has an equal and opposite energy potential. This is the result of a zero-energy energy level.
In free energy potential energy, it is assumed that the system will evolve at a rate that is not increasing, and will be in equilibrium with each other (or at least, be well matched) in the long term. A system moving at a constant velocity (that is constant) will not deviate from this equilibrium.
The concept of free energy potential energy is used most commonly in the physical sciences to describe the energy of a system. In this context, the FEPE is given as the energy of a system that was in equilibrium at some point in time.
Free Energy Equivalence
It is often claimed by critics that free energy potential energy is zero because, in a non-equilibrium system, the energy potential energy is zero. However, it is also possible to find FEPE values for a system with no interaction with any external medium, where energy is conserved.
For the systems described in this chapter, the “equilibrium” point of time (the point where the total energy of the system does not change) for the free energy potential energy is defined as the point at which the total energy of the system does not decrease. When an external medium is present, then the free energy potential energy increases by an amount equal to the difference between the net energy of the system at that point in time and the amount of available energy from any change in energy from that area of the system.
A further complication arises, however, because of the role that the interaction might play in determining whether the equilibrium point
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