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DETERMINING POTENTIEL ENERGY VALUES Potential is the specific potential energy. That is, when potential energy depends on some quantity associated with object in question, potential is potential energy per unit of that quantity. For example, gravitational potential is gravitational potential energy per unit of mass. Electrostatic potential is the electrostatic potential energy per unit of charge. The nature of potential is that the zero point is arbitrary; it can be set like the origin of a coordinate system. That is not to say that it is insignificant; once the zero of potential is set, then every value of potential is measured with respect to that zero. Another way of saying it is that it is the change in potential which has physical significance. The zero of electric potential (voltage) is set for convenience, but there is usually some physical or geometric logic to the choice of the zero point. For a single point charge or localized collection of charges, it is logical to set the zero point at infinity. But for an infinite line charge, that is not a logical choice, since the local values of potential would go to infinity. For practical electrical circuits, the earth or ground potential is usually taken to be zero and everything is referenced to the earth. Gravitional potential energy We first consider a particle with mass m moving vertically along a y axis (the positive direction is upward). As the particle moves from point yi to point yf, in the gravitational force Fg does work on it. To find the corresponding change in the gravitational potential energy of the particle-Earth system, we use the below equation. In this equation we integrate along y axis instead of x axis because the gravitational force acts vertically and we substitute –mg for the force symbol F, because Fg has the magnitude mg and is directed down the y axis. Only changes ∆U in gravitational potential energy (or any other type of potential energy) are physically meaningful. However , to simplify a calculation or a discussion , we sometimes would like say that a certain gravitational potential value U is associated with certain particle-Earth system when the particle is at a certain height y. to do so, we rewrite equation Then we take the Ui to be the gravitational potential energy of the system when it is in reference configuration in which the particles is at a reference point yi . usually we take UI =0. Doing this changes the equation Elastic potential energy First, we consider the block-spring system shown in the figure, with the block moving on the end of a spring of spring constant k.As the block moves from point xi to point xf, the spring force Fx= -kx does work on the block. To find the corresponding s change in the elastic potential energy of the block-spring system, we substitute –kx for F(x) in the below equation To associate a potential energy value U with the block at the position x, we choose the reference configuration to be when the spring is its relaxed length and the block is at xi = 0. Then the elastic potential energy Ui is 0, and the equation becomes which gives us Electric potential energy Potential energy can be defined as the capacity for doing work which arises from position or configuration. In the electrical case, a charge will exert a force on any other charge and potential energy arises from any collection of charges. For example, if a positive charge Q is fixed at some point in space, any other positive charge which is brought close to it will experience a repulsive force and will therefore have potential energy. The potential energy of a test charge q in the vicinity of this source charge will be: The general expression for the electric potential as a result of a point charge Q can be obtained by referencing to a zero of potential at infinity. In electricity, it is usually more convenient to use the electric potential energy per unit charge, just called electric potential or voltage. Difference between electrostatic potentials between two points is the voltage. Voltage is the amount of potential energy change for 1 coulomb of charge moving from first point to the second. If you have a vacuum tube, effectively giving you no resistance, an electron traveling across 1V gap would gain kinetic energy equal to potential energy drop, which is the charge of electron * 1V, or in units of electron charge, this is energy of 1 electron-volt (eV). In a circuit, however, all this energy is dissipated as heat. If one coulomb of charge moves across 1V of potential, 1J of heat has been produced. Since current is charge flow per unit time, current time voltage gives you amount of energy going into heat per unit of time, or power.