Potential energy


In the case of a bow and arrow, the energy is converted from the potential energy in the archer's arm to the potential energy in the bent limbs of the bow when the string is drawn back. When the string is released, the potential energy in the bow limbs is transferred back through the string to become kinetic energy in the arrow as it takes flight.

Common symbol(s): 
PE, U, or V

SI unit: 
joule (J)

Derivations from other quantities: 
U = m · g · h (gravitational)
U = ½ · k · x^{2} (elastic)
U = C · V^{2} / 2 (electric)
U = m · B (magnetic)

In physics, potential energy is the energy of an object or a system due to the position of the body or the arrangement of the particles of the system.^{[1]}
The SI unit for measuring work and energy is the joule (symbol J).
The term potential energy was coined by the 19th century Scottish engineer and physicist William Rankine,^{[2]}^{[3]} although it has links to Greek philosopher Aristotle's concept of potentiality.
Potential energy is associated with a set of forces that act on a body in a way that depends only on the body's position in space. This allows the set of forces to be considered as having a specified vector at every point in space forming what is known as a vector field of forces, or a force field. If the work of forces of this type acting on a body that moves from a start to an end position is defined only by these two positions and does not depend on the trajectory of the body between the two, then there is a function known as a potential that can be evaluated at the two positions to determine this work. Furthermore, the force field is defined by this potential function, also called potential energy.
Overview
Potential energy is often associated with restoring forces such as a spring or the force of gravity. The action of stretching the spring or lifting the mass is performed by an external force that works against the force field of the potential. This work is stored in the force field, which is said to be stored as potential energy. If the external force is removed the force field acts on the body to perform the work as it moves the body back to the initial position, reducing the stretch of the spring or causing a body to fall.
The more formal definition is that potential energy is the energy difference between the energy of an object in a given position and its energy at a reference position.
There are various types of potential energy, each associated with a particular type of force. More specifically, every conservative force gives rise to potential energy. For example, the work of an elastic force is called elastic potential energy; work of the gravitational force is called gravitational potential energy; work of the Coulomb force is called electric potential energy; work of the strong nuclear force or weak nuclear force acting on the baryon charge is called nuclear potential energy; work of intermolecular forces is called intermolecular potential energy. Chemical potential energy, such as the energy stored in fossil fuels, is the work of the Coulomb force during rearrangement of mutual positions of electrons and nuclei in atoms and molecules. Thermal energy usually has two components: the kinetic energy of random motions of particles and the potential energy of their mutual positions.
As a general rule, the work done by a conservative force F will be
 $\backslash ,W\; =\; \backslash Delta\; U$
where $\backslash Delta\; U$ is the change in the potential energy associated with that particular force. Common notations for potential energy are U, V, and E_{p}.
Work and potential energy
The work of a force acting on a moving body yields a difference in potential energy when the integration of the work is path independent. The scalar product of a force F and the velocity v of its point of application defines the power input to a system at an instant of time. Integration of this power over the trajectory of the point of application, d=x(t), defines the work input to the system by the force.
If the work for an applied force is independent of the path, then the work done by the force is evaluated at the start and end of the trajectory of the point of application. This means that there is a function U (x), called a "potential," that can be evaluated at the two points x(t_{1}) and x(t_{2}) to obtain the work over any trajectory between these two points. It is tradition to define this function with a negative sign so that positive work is a reduction in the potential, that is
 $W\; =\; \backslash int\_C\; \backslash bold\{F\}\; \backslash cdot\; \backslash mathrm\{d\}\backslash bold\{x\}\; =\; \backslash int\_\{\backslash mathbf\{x\}(t\_1)\}^\{\backslash mathbf\{x\}(t\_2)\}\; \backslash bold\{F\}\; \backslash cdot\; \backslash mathrm\{d\}\backslash bold\{x\}\; =\; U(\backslash mathbf\{x\}(t\_1))U(\backslash mathbf\{x\}(t\_2)).$
The function U(x) is called the potential energy associated with the applied force. Examples of forces that have potential energies are gravity and spring forces.
In this case, the application of the del operator to the work function yields
 $\{\backslash nabla\; W\}\; =\; \{\backslash nabla\; U\}\; =\; \backslash left\; (\; \backslash frac\{\backslash partial\; U\}\{\backslash partial\; x\},\; \backslash frac\{\backslash partial\; U\}\{\backslash partial\; y\},\; \backslash frac\{\backslash partial\; U\}\{\backslash partial\; z\}\; \backslash right\; )\; =\; \backslash mathbf\{F\},$
and the force F is said to be "derivable from a potential."^{[4]}
Because the potential U defines a force F at every point x in space, the set of forces is called a force field. The power applied to a body by a force field is obtained from the gradient of the work, or potential, in the direction of the velocity V of the body, that is
 $P(t)\; =\; \{\backslash nabla\; U\}\; \backslash cdot\; \backslash mathbf\{v\}\; =\; \backslash mathbf\{F\}\backslash cdot\backslash mathbf\{v\}.$
Examples of work that can be computed from potential functions are gravity and spring forces.^{[5]}
Potential function for near Earth gravity
In classical physics, gravity exerts a constant downward force F=(0, 0, F_{z}) on the center of mass of a body moving near the surface of the Earth. The work of gravity on a body moving along a trajectory s(t) = (x(t), y(t), z(t)), such as the track of a roller coaster is calculated using its velocity, v=(v_{x}, v_{y}, v_{z}), to obtain
 $W=\backslash int\_\{t\_1\}^\{t\_2\}\backslash boldsymbol\{F\}\backslash cdot\backslash boldsymbol\{v\}dt\; =\; \backslash int\_\{t\_1\}^\{t\_2\}F\_z\; v\_z\; dt\; =\; F\_z\backslash Delta\; z.$
where the integral of the vertical component of velocity is the vertical distance. Notice that the work of gravity depends only on the vertical movement of the curve s(t).
The function U(s)=mgh is called the potential energy of a near earth gravity field.
Potential function for a linear spring
A horizontal spring exerts a force F=(kx, 0, 0) that is proportional to its deflection in the x direction. The work of this spring on a body moving along the space curve s(t) = (x(t), y(t), z(t)), is calculated using its velocity, v=(v_{x}, v_{y}, v_{z}), to obtain
 $W=\backslash int\_0^t\backslash boldsymbol\{F\}\backslash cdot\backslash boldsymbol\{v\}dt\; =\backslash int\_0^tkx\; v\_x\; dt\; =\; \backslash frac\{1\}\{2\}kx^2.$
For convenience, consider contact with the spring occurs at t = 0, then the integral of the product of the distance x and the xvelocity, xv_{x}, is (1/2)x^{2}.
The function U(x)= 1/2 kx^{2} is called the potential energy of a linear spring.
Reference level
The potential energy is a function of the state a system is in, and is defined relative to that for a particular state. This reference state is not always a real state, it may also be a limit, such as with the distances between all bodies tending to infinity, provided that the energy involved in tending to that limit is finite, such as in the case of inversesquare law forces. Any arbitrary reference state could be used, therefore it can be chosen based on convenience.
Typically the potential energy of a system depends on the relative positions of its components only, so the reference state can also be expressed in terms of relative positions.
Gravitational potential energy
Gravitational energy is the potential energy associated with gravitational force, as work is required to elevate objects against Earth's gravity. The potential energy due to elevated positions is called gravitational potential energy, and is evidenced by water in an elevated reservoir or kept behind a dam. If an object falls from one point to another point inside a gravitational field, the force of gravity will do positive work on the object, and the gravitational potential energy will decrease by the same amount.
Consider a book placed on top of a table. As the book is raised from the floor, to the table, some external force works against the gravitational force. If the book falls back to the floor, the "falling" energy the book receives is provided by the gravitational force. Thus, if the book falls off the table, this potential energy goes to accelerate the mass of the book and is converted into kinetic energy. When the book hits the floor this kinetic energy is converted into heat and sound by the impact.
The factors that affect an object's gravitational potential energy are its height relative to some reference point, its mass, and the strength of the gravitational field it is in. Thus, a book lying on a table has less gravitational potential energy than the same book on top of a taller cupboard, and less gravitational potential energy than a heavier book lying on the same table. An object at a certain height above the Moon's surface has less gravitational potential energy than at the same height above the Earth's surface because the Moon's gravity is weaker. Note that "height" in the common sense of the term cannot be used for gravitational potential energy calculations when gravity is not assumed to be a constant. The following sections provide more detail.
Local approximation
The strength of a gravitational field varies with location. However, when the change of distance is small in relation to the distances from the center of the source of the gravitational field, this variation in field strength is negligible and we can assume that the force of gravity on a particular object is constant. Near the surface of the Earth, for example, we assume that the acceleration due to gravity is a constant g = 9.8 m/s^{2} ("standard gravity"). In this case, a simple expression for gravitational potential energy can be derived using the W = Fd equation for work, and the equation
 $W\_F\; =\; \backslash Delta\; U\_F.\backslash !$
The amount of gravitational potential energy possessed by an elevated object is equal to the work done against gravity in lifting it. The work done equals the force required to move it upward multiplied with the vertical distance it is moved (remember W = Fd). The upward force required while moving at a constant velocity is equal to the weight, mg, of an object, so the work done in lifting it through a height h is the product mgh. Thus, when accounting only for mass, gravity, and altitude, the equation is:^{[6]}
 $U\; =\; mgh\backslash !$
where U is the potential energy of the object relative to its being on the Earth's surface, m is the mass of the object, g is the acceleration due to gravity, and h is the altitude of the object.^{[7]} If m is expressed in kilograms, g in m/s^{2} and h in metres then U will be calculated in joules.
Hence, the potential difference is
 $\backslash ,\backslash Delta\; U\; =\; mg\; \backslash Delta\; h.\backslash $
General formula
However, over large variations in distance, the approximation that g is constant is no longer valid, and we have to use calculus and the general mathematical definition of work to determine gravitational potential energy. For the computation of the potential energy we can integrate the gravitational force, whose magnitude is given by Newton's law of gravitation, with respect to the distance r between the two bodies. Using that definition, the gravitational potential energy of a system of masses m_{1} and M_{2} at a distance r using gravitational constant G is
 $U\; =\; G\; \backslash frac\{m\_1\; M\_2\}\{r\}\backslash \; +\; K$,
where K is the constant of integration. Choosing the convention that K=0 makes calculations simpler, albeit at the cost of making U negative; for why this is physically reasonable, see below.
Given this formula for U, the total potential energy of a system of n bodies is found by summing, for all $\backslash frac\{n\; (\; n\; \; 1\; )\}\{2\}$ pairs of two bodies, the potential energy of the system of those two bodies.
Considering the system of bodies as the combined set of small particles the bodies consist of, and applying the previous on the particle level we get the negative gravitational binding energy. This potential energy is more strongly negative than the total potential energy of the system of bodies as such since it also includes the negative gravitational binding energy of each body. The potential energy of the system of bodies as such is the negative of the energy needed to separate the bodies from each other to infinity, while the gravitational binding energy is the energy needed to separate all particles from each other to infinity.
 $U\; =\; \; m\; \backslash left(G\; \backslash frac\{\; M\_1\}\{r\_1\}+\; G\; \backslash frac\{\; M\_2\}\{r\_2\}\backslash right)$
therefore,
 $U\; =\; \; m\; \backslash sum\; G\; \backslash frac\{\; M\}\{r\}$,
Why choose a convention where gravitational energy is negative?
As with all potential energies, only differences in gravitational potential energy matter for most physical purposes, and the choice of zero point is arbitrary. Given that there is no reasonable criterion for preferring one particular finite r over another, there seem to be only two reasonable choices for the distance at which U becomes zero: $r=0$ and $r=\backslash infty$. The choice of $U=0$ at infinity may seem peculiar, and the consequence that gravitational energy is always negative may seem counterintuitive, but this choice allows gravitational potential energy values to be finite, albeit negative.
The singularity at $r=0$ in the formula for gravitational potential energy means that the only other apparently reasonable alternative choice of convention, with $U=0$ for $r=0$, would result in potential energy being positive, but infinitely large for all nonzero values of r, and would make calculations involving sums or differences of potential energies beyond what is possible with the real number system. Since physicists abhor infinities in their calculations, and r is always nonzero in practice, the choice of $U=0$ at infinity is by far the more preferable choice, even if the idea of negative energy in a gravity well appears to be peculiar at first.
The negative value for gravitational energy also has deeper implications that make it seem more reasonable in cosmological calculations where the total energy of the universe can meaningfully be considered; see inflation theory for more on this.
Uses
Gravitational potential energy has a number of practical uses, notably the generation of hydroelectricity. For example in Dinorwig, Wales, there are two lakes, one at a higher elevation than the other. At times when surplus electricity is not required (and so is comparatively cheap), water is pumped up to the higher lake, thus converting the electrical energy (running the pump) to gravitational potential energy. At times of peak demand for electricity, the water flows back down through electrical generator turbines, converting the potential energy into kinetic energy and then back into electricity. (The process is not completely efficient and some of the original energy from the surplus electricity is in fact lost to friction.) See also pumped storage.
Gravitational potential energy is also used to power clocks in which falling weights operate the mechanism.
It's also used by
counterweights for lifting up an
Elevator, crane, or
Sash window.
Roller coasters are an entertaining way to utilize potential energy  chains are used to move a car up an incline (building up gravitational potential energy), to then have that energy converted into kinetic energy as it falls.
Another practical use is utilizing gravitational potential energy to descend (perhaps coast) downhill in transportation such as the descent of an automobile, truck, railroad train, bicycle, airplane, or fluid in a pipeline. In some cases the Kinetic energy obtained from potential energy of descent may be used to start ascending the next grade such as what happens when a road is undulating and has frequent dips.
Elastic potential energy
Elastic potential energy is the potential energy of an elastic object (for example a bow or a catapult) that is deformed under tension or compression (or stressed in formal terminology). It arises as a consequence of a force that tries to restore the object to its original shape, which is most often the electromagnetic force between the atoms and molecules that constitute the object. If the stretch is released, the energy is transformed into kinetic energy.
Calculation of elastic potential energy
The elastic potential energy stored in a stretched spring can be calculated by finding the work necessary to stretch the spring a distance x from its unstretched length:
 $U\; =\; \backslash int\backslash vec\{F\}\backslash cdot\; d\backslash vec\{x\}$
an ideal spring will follow Hooke's Law:
 $F=k\; \backslash Delta\; x\backslash ,$
The work done (and therefore the stored potential energy) will then be:
 $U\; =\; \backslash int\backslash vec\{F\}\backslash cdot\; d\backslash vec\{x\}=\backslash int\; \{k\; x\}\backslash ,\; dx\; =\; \backslash frac\; \{1\}\; \{2\}\; k\; x^2.$
The units are in joules (J).
The equation is often used in calculations of positions of mechanical equilibrium. This equation can also be stated as:
 $U\; =\; \backslash frac\{1\}\{2\}k\; \backslash Delta\; x^2\backslash ,$
Chemical potential energy
Chemical potential energy is a form of potential energy related to the structural arrangement of atoms or molecules. This arrangement may be the result of chemical bonds within a molecule or otherwise. Chemical energy of a chemical substance can be transformed to other forms of energy by a chemical reaction. As an example, when a fuel is burned the chemical energy is converted to heat, same is the case with digestion of food metabolized in a biological organism. Green plants transform solar energy to chemical energy through the process known as photosynthesis, and electrical energy can be converted to chemical energy through electrochemical reactions.
The similar term chemical potential is used to indicate the potential of a substance to undergo a change of configuration, be it in the form of a chemical reaction, spatial transport, particle exchange with a reservoir, etc.
Electric potential energy
An object can have potential energy by virtue of its electric charge and several forces related to their presence. There are two main types of this kind of potential energy: electrostatic potential energy, electrodynamic potential energy (also sometimes called magnetic potential energy).
Electrostatic potential energy
In case the electric charge of an object can be assumed to be at rest, it has potential energy due to its position relative to other charged objects.
The electrostatic potential energy is the energy of an electrically charged particle (at rest) in an electric field. It is defined as the work that must be done to move it from an infinite distance away to its present location, adjusted for nonelectrical forces on the object. This energy will generally be nonzero if there is another electrically charged object nearby.
The simplest example is the case of two pointlike objects A_{1} and A_{2} with electrical charges q_{1} and q_{2}. The work W required to move A_{1} from an infinite distance to a distance r away from A_{2} is given by:
 $W=\backslash frac\{1\}\{4\backslash pi\backslash varepsilon\_0\}\backslash frac\{q\_1q\_2\}\{r\},$
where ε_{0} is the vacuum permittivity. This may also be written using Coulomb's constant k_{e} = 1 ⁄ 4πε_{0}.
This equation may be obtained by integrating the Coulomb force between the limits of infinity and r.
A related quantity called electric potential (commonly denoted with a V for voltage) is equal to the electric potential energy per unit charge.
Magnetic potential energy
The energy of a magnetic moment m in an externally produced magnetic Bfield B has potential energy^{[8]}
 $U=\backslash mathbf\{m\}\backslash cdot\backslash mathbf\{B\}.$
The magnetization M in a field is
 $U\; =\; \backslash frac\{1\}\{2\}\backslash int\; \backslash mathbf\{M\}\backslash cdot\backslash mathbf\{B\}\; dV,$
where the integral can be over all space or, equivalently, where M is nonzero.^{[9]}
Magnetic potential energy is the form of energy related not only to the distance between magnetic materials, but also to the orientation, or alignment, of those materials within the field. For example, the needle of a compass has the lowest magnetic potential energy when it is aligned with the north and south poles of the Earth's magnetic field. If the needle is moved by an outside force, torque is exerted on the magnetic dipole of the needle by the Earth's magnetic field, causing it to move back into alignment. The magnetic potential energy of the needle is highest when it is perpendicular to the Earth's magnetic field. Two magnets will have potential energy in relation to each other and the distance between them, but this also depends on their orientation. If the opposite poles are held apart, the potential energy will be the highest when they are near the edge of their attraction, and the lowest when they pull together. Conversely, like poles will have the highest potential energy when forced together, and the lowest when they spring apart.^{[10]}^{[11]}
Nuclear potential energy
Nuclear potential energy is the potential energy of the particles inside an atomic nucleus. The nuclear particles are bound together by the strong nuclear force. Weak nuclear forces provide the potential energy for certain kinds of radioactive decay, such as beta decay.
Nuclear particles like protons and neutrons are not destroyed in fission and fusion processes, but collections of them have less mass than if they were individually free, and this mass difference is liberated as heat and radiation in nuclear reactions (the heat and radiation have the missing mass, but it often escapes from the system, where it is not measured). The energy from the Sun is an example of this form of energy conversion. In the Sun, the process of hydrogen fusion converts about 4 million tonnes of solar matter per second into electromagnetic energy, which is radiated into space.
Relation between potential energy, potential and force
Potential energy is closely linked with forces. If the work done moving along a path which starts and ends in the same location is zero, then the force is said to be conservative and it is possible to define a numerical value of potential associated with every point in space. A force field can be reobtained by taking the negative of the vector gradient of the potential field.
For example, gravity is a conservative force. The associated potential is the gravitational potential, often denoted by $\backslash phi$ or $V$, corresponding to the energy per unit mass as a function of position. The gravitational potential energy of two particles of mass M and m separated by a distance r is
 $U\; =\; \backslash frac\{G\; M\; m\}\{r\},$
The gravitational potential (specific energy) of the two bodies is
 $\backslash phi\; =\; \backslash left(\; \backslash frac\{GM\}\{r\}\; +\; \backslash frac\{Gm\}\{r\}\; \backslash right)=\; \backslash frac\{G(M+m)\}\{r\}\; =\; \backslash frac\{GMm\}\{\backslash mu\; r\}\; =\; \backslash frac\{U\}\{\backslash mu\}.$
where $\backslash mu$ is the reduced mass.
The work done against gravity by moving an infinitesimal mass from point A with $U\; =\; a$ to point B with $U\; =\; b$ is $(b\; \; a)$ and the work done going back the other way is $(a\; \; b)$ so that the total work done in moving from A to B and returning to A is
 $U\_\{A\; \backslash to\; B\; \backslash to\; A\}\; =\; (b\; \; a)\; +\; (a\; \; b)\; =\; 0.\; \backslash ,$
If the potential is redefined at A to be $a\; +\; c$ and the potential at B to be $b\; +\; c$, where $c$ is a constant (i.e. $c$ can be any number, positive or negative, but it must be the same at A as it is at B) then the work done going from A to B is
 $U\_\{A\; \backslash to\; B\}\; =\; (b\; +\; c)\; \; (a\; +\; c)\; =\; b\; \; a\; \backslash ,$
as before.
In practical terms, this means that one can set the zero of $U$ and $\backslash phi$ anywhere one likes. One may set it to be zero at the surface of the Earth, or may find it more convenient to set zero at infinity (as in the expressions given earlier in this section).
A thing to note about conservative forces is that the work done going from A to B does not depend on the route taken. If it did then it would be pointless to define a potential at each point in space. An example of a nonconservative force is friction. With friction, the route taken does affect the amount of work done, and it makes little sense to define a potential associated with friction.
All the examples above are actually force field stored energy (sometimes in disguise). For example in elastic potential energy, stretching an elastic material forces the atoms very slightly further apart. The equilibrium between electromagnetic forces and Pauli repulsion of electrons (they are fermions obeying Fermi statistics) is slightly violated resulting in a small returning force. Scientists rarely discuss forces on an atomic scale. Often interactions are described in terms of energy rather than force. One may think of potential energy as being derived from force or think of force as being derived from potential energy (though the latter approach requires a definition of energy that is independent from force which does not currently exist).
A conservative force can be expressed in the language of differential geometry as a closed form. As Euclidean space is contractible, its de Rham cohomology vanishes, so every closed form is also an exact form, and can be expressed as the gradient of a scalar field. This gives a mathematical justification of the fact that all conservative forces are gradients of a potential field.
Notes
References
External links
 What is potential energy?
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