Electrostatics - wikipedia Electrostatics For a less technical introduction, see Static electricity. Electromagnetism Electricity Magnetism Electrostatics Electric charge Static electricity Electric field Conductor Insulator Triboelectricity Electrostatic discharge Induction Coulomb 's law Gauss 's law Electric flux / potential energy Electric dipole moment Polarization density Magnetostatics Ampère 's law Magnetic field Magnetization Magnetic flux Biot -- Savart law Magnetic dipole moment Gauss 's law for magnetism Electrodynamics Lorentz force law Electromagnetic induction Faraday 's law Lenz 's law Displacement current Magnetic potential Maxwell 's equations Electromagnetic field Electromagnetic pulse Electromagnetic radiation Maxwell tensor Poynting vector Liénard -- Wiechert potential Jefimenko 's equations Eddy current London equations Mathematical descriptions of the electromagnetic field Electrical network Electric current Electric potential Voltage Resistance Ohm 's law Series circuit Parallel circuit Direct current Alternating current Electromotive force Capacitance Inductance Impedance Resonant cavities Waveguides Covariant formulation Electromagnetic tensor ( stress -- energy tensor ) Four - current Electromagnetic four - potential Scientists Ampère Coulomb Faraday Gauss Heaviside Henry Hertz Lorentz Maxwell Tesla Volta Weber Ørsted Paper strips attracted by a charged CD Styrofoam peanuts clinging to a cat 's fur due to static electricity. The triboelectric effect causes an electrostatic charge to build up on the fur due to the cat 's motions. The electric field of the charge causes polarization of the molecules of the styrofoam due to electrostatic induction, resulting in a slight attraction of the light plastic pieces to the charged fur. This is also the cause of static cling in clothes. Electrostatics is a branch of physics that deals with study of the electric charges at rest. Since classical physics, it has been known that some materials such as amber attract lightweight particles after rubbing. The Greek word for amber, ήλεκτρον, or electron, was the source of the word ' electricity '. Electrostatic phenomena arise from the forces that electric charges exert on each other. Such forces are described by Coulomb 's law. Even though electrostatically induced forces seem to be rather weak, some electrostatic forces such as the one between an electron and a proton, that together make up a hydrogen atom, is about 36 orders of magnitude stronger than the gravitational force acting between them. There are many examples of electrostatic phenomena, from those as simple as the attraction of the plastic wrap to your hand after you remove it from a package to the apparently spontaneous explosion of grain silos, the damage of electronic components during manufacturing, and photocopier & laser printer operation. Electrostatics involves the buildup of charge on the surface of objects due to contact with other surfaces. Although charge exchange happens whenever any two surfaces contact and separate, the effects of charge exchange are usually only noticed when at least one of the surfaces has a high resistance to electrical flow. This is because the charges that transfer are trapped there for a time long enough for their effects to be observed. These charges then remain on the object until they either bleed off to ground or are quickly neutralized by a discharge : e.g., the familiar phenomenon of a static ' shock ' is caused by the neutralization of charge built up in the body from contact with insulated surfaces. Contents 1 Coulomb 's law 2 Electric field 2.1 Gauss 's law 2.2 Poisson and Laplace equations 3 Electrostatic approximation 3.1 Electrostatic potential 3.2 Electrostatic energy 3.3 Electrostatic pressure 4 Triboelectric series 5 Electrostatic generators 6 Charge neutralization 7 Electrostatic induction 8 ' Static ' electricity 8.1 Static electricity and chemical industry 8.1. 1 Applicable standards 9 Electrostatic induction in commercial applications 10 See also 11 References 12 Further reading 13 External links Coulomb 's law Main article : Coulomb 's law We begin with the magnitude of the electrostatic force ( in newtons ) between two point charges q ( displaystyle q ) and Q ( displaystyle Q ) ( in coulombs ). It is convenient to label one of these charges, q ( displaystyle q ), as a test charge, and call Q ( displaystyle Q ) a source charge. As we develop the theory, more source charges will be added. If r ( displaystyle r ) is the distance ( in meters ) between two charges, then the force is : F = 1 4 π ε 0 q Q r 2 = k e q Q r 2, ( displaystyle F = ( \frac ( 1 ) ( 4 pi \varepsilon _ ( 0 ) ) ) ( \frac ( qQ ) ( r ^ ( 2 ) ) ) = k_ ( e ) ( \frac ( qQ ) ( r ^ ( 2 ) ) ) ,, ) where ε is the vacuum permittivity, or permittivity of free space : ε 0 ≈ 10 − 9 36 π C 2 N − 1 m − 2 ≈ 8.854 187 817 × 10 − 12 C 2 N − 1 m − 2. ( displaystyle \varepsilon _ ( 0 ) approx ( 10 ^ ( - 9 ) over 36 pi ) ; ; mathrm ( C ^ ( 2 ) \N ^ ( - 1 ) m ^ ( - 2 ) ) approx 8.854 187 817 \times 10 ^ ( - 12 ) ; ; mathrm ( C ^ ( 2 ) \N ^ ( - 1 ) m ^ ( - 2 ) ). ) The SI units of ε are equivalently A s kg m or C N m or F m. Coulomb 's constant is : k e ≈ 1 4 π ε 0 ≈ 8.987 551 787 × 10 9 N m 2 C − 2. ( displaystyle k_ ( e ) approx ( \frac ( 1 ) ( 4 pi \varepsilon _ ( 0 ) ) ) approx 8.987 551 787 \times 10 ^ ( 9 ) ; ; mathrm ( N m ^ ( 2 ) C ) ^ ( - 2 ). ) The use of ε instead of k in expressing Coulomb 's Law is related to the fact that the force is inversely proportional to the surface area of a sphere with radius equal to the separation between the two charges. A single proton has a charge of e, and the electron has a charge of − e, where, e ≈ 1.602 176 565 × 10 − 19 C. ( displaystyle e approx 1.602 176 565 \times 10 ^ ( - 19 ) ; ; mathrm ( C ). ) These physical constants ( ε, k, e ) are currently defined so that ε and k are exactly defined, and e is a measured quantity. Electric field The electrostatic field ( lines with arrows ) of a nearby positive charge ( + ) causes the mobile charges in conductive objects to separate due to electrostatic induction. Negative charges ( blue ) are attracted and move to the surface of the object facing the external charge. Positive charges ( red ) are repelled and move to the surface facing away. These induced surface charges are exactly the right size and shape so their opposing electric field cancels the electric field of the external charge throughout the interior of the metal. Therefore, the electrostatic field everywhere inside a conductive object is zero, and the electrostatic potential is constant. The electric field, E → ( displaystyle ( \vec ( E ) ) ), in units of newtons per coulomb or volts per meter, is a vector field that can be defined everywhere, except at the location of point charges ( where it diverges to infinity ). It is defined as the electrostatic force F → ( displaystyle ( \vec ( F ) ) , ) in newtons on a hypothetical small test charge at the point due to Coulomb 's Law, divided by the magnitude of the charge q ( displaystyle q , ) in coulombs E → = F → q ( displaystyle ( \vec ( E ) ) = ( ( \vec ( F ) ) over q ) , ) Electric field lines are useful for visualizing the electric field. Field lines begin on positive charge and terminate on negative charge. They are parallel to the direction of the electric field at each point, and the density of these field lines is a measure of the magnitude of the electric field at any given point. Consider a collection of N ( displaystyle N ) particles of charge Q i ( displaystyle Q_ ( i ) ), located at points r → i ( displaystyle ( \vec ( r ) ) _ ( i ) ) ( called source points ), the electric field at r → ( displaystyle ( \vec ( r ) ) ) ( called the field point ) is : E → ( r → ) = 1 4 π ε 0 ∑ i = 1 N R ^ i Q i ∥ R → i ∥ 2, ( displaystyle ( \vec ( E ) ) ( ( \vec ( r ) ) ) = ( \frac ( 1 ) ( 4 pi \varepsilon _ ( 0 ) ) ) sum _ ( i = 1 ) ^ ( N ) ( \frac ( ( widehat ( mathcal ( R ) ) ) _ ( i ) Q_ ( i ) ) ( left ( mathcal ( \vec ( R ) ) ) _ ( i ) \right ^ ( 2 ) ) ), ) where R → i = r → − r → i, ( displaystyle ( \vec ( mathcal ( R ) ) ) _ ( i ) = ( \vec ( r ) ) - ( \vec ( r ) ) _ ( i ), ) is the displacement vector from a source point r → i ( displaystyle ( \vec ( r ) ) _ ( i ) ) to the field point r → ( displaystyle ( \vec ( r ) ) ), and R ^ i = R → i / ∥ R → i ∥ ( displaystyle ( widehat ( mathcal ( R ) ) ) _ ( i ) = ( \vec ( mathcal ( R ) ) ) _ ( i ) / left ( \vec ( mathcal ( R ) ) ) _ ( i ) \right ) is a unit vector that indicates the direction of the field. For a single point charge at the origin, the magnitude of this electric field is E = k e Q / R 2, ( displaystyle E = k_ ( e ) Q / ( mathcal ( R ) ) ^ ( 2 ), ) and points away from that charge is positive. The fact that the force ( and hence the field ) can be calculated by summing over all the contributions due to individual source particles is an example of the superposition principle. The electric field produced by a distribution of charges is given by the volume charge density ρ ( r → ) ( displaystyle \rho ( ( \vec ( r ) ) ) ) and can be obtained by converting this sum into a triple integral : E → ( r → ) = 1 4 π ε 0 ∫∫∫ r → − r → ′ ∥ r → − r → ′ ∥ 3 ρ ( r → ′ ) d 3 ⁡ r ′ ( displaystyle ( \vec ( E ) ) ( ( \vec ( r ) ) ) = ( \frac ( 1 ) ( 4 pi \varepsilon _ ( 0 ) ) ) iiint ( \frac ( ( \vec ( r ) ) - ( \vec ( r ) ) , ' ) ( left ( \vec ( r ) ) - ( \vec ( r ) ) , ' \right ^ ( 3 ) ) ) \rho ( ( \vec ( r ) ) , ' ) operatorname ( d ) ^ ( 3 ) r , ' ) Gauss 's law Gauss 's law states that `` the total electric flux through any closed surface in free space of any shape drawn in an electric field is proportional to the total electric charge enclosed by the surface. '' Mathematically, Gauss 's law takes the form of an integral equation : ∮ S E → ⋅ d A → = 1 ε 0 Q e n c l o s e d = ∫ V ρ ε 0 ⋅ d 3 ⁡ r, ( displaystyle oint _ ( S ) ( \vec ( E ) ) cdot mathrm ( d ) ( \vec ( A ) ) = ( \frac ( 1 ) ( \varepsilon _ ( 0 ) ) ) , Q_ ( enclosed ) = int _ ( V ) ( \rho over \varepsilon _ ( 0 ) ) cdot operatorname ( d ) ^ ( 3 ) r, ) where d 3 ⁡ r = d x d y d z ( displaystyle operatorname ( d ) ^ ( 3 ) r = mathrm ( d ) x mathrm ( d ) y mathrm ( d ) z ) is a volume element. If the charge is distributed over a surface or along a line, replace ρ d 3 r ( displaystyle \rho mathrm ( d ) ^ ( 3 ) r ) by σ d A ( displaystyle sigma mathrm ( d ) A ) or λ d l ( displaystyle lambda mathrm ( d ) ell ). The Divergence Theorem allows Gauss 's Law to be written in differential form : ∇ → ⋅ E → = ρ ε 0. ( displaystyle ( \vec ( \nabla ) ) cdot ( \vec ( E ) ) = ( \rho over \varepsilon _ ( 0 ) ). ) where ∇ → ⋅ ( displaystyle ( \vec ( \nabla ) ) cdot ) is the divergence operator. Poisson and Laplace equations The definition of electrostatic potential, combined with the differential form of Gauss 's law ( above ), provides a relationship between the potential Φ and the charge density ρ : ∇ 2 φ = − ρ ε 0. ( displaystyle ( \nabla ) ^ ( 2 ) phi = - ( \rho over \varepsilon _ ( 0 ) ). ) This relationship is a form of Poisson 's equation. In the absence of unpaired electric charge, the equation becomes Laplace 's equation : ∇ 2 φ = 0, ( displaystyle ( \nabla ) ^ ( 2 ) phi = 0, ) Electrostatic approximation The validity of the electrostatic approximation rests on the assumption that the electric field is irrotational : ∇ → × E → = 0. ( displaystyle ( \vec ( \nabla ) ) \times ( \vec ( E ) ) = 0. ) From Faraday 's law, this assumption implies the absence or near - absence of time - varying magnetic fields : ∂ B → ∂ t = 0. ( displaystyle ( partial ( \vec ( B ) ) over partial t ) = 0. ) In other words, electrostatics does not require the absence of magnetic fields or electric currents. Rather, if magnetic fields or electric currents do exist, they must not change with time, or in the worst - case, they must change with time only very slowly. In some problems, both electrostatics and magnetostatics may be required for accurate predictions, but the coupling between the two can still be ignored. Electrostatics and magnetostatics can both be seen as Galilean limits for electromagnetism. Electrostatic potential Because the electric field is irrotational, it is possible to express the electric field as the gradient of a scalar function, φ ( displaystyle phi ), called the electrostatic potential ( also known as the voltage ). An electric field, E ( displaystyle E ), points from regions of high electric potential to regions of low electric potential, expressed mathematically as E → = − ∇ → φ. ( displaystyle ( \vec ( E ) ) = - ( \vec ( \nabla ) ) phi. ) The Gradient Theorem can be used to establish that the electrostatic potential is the amount of work per unit charge required to move a charge from point a ( displaystyle a ) to point b ( displaystyle b ) with the following line integral : − ∫ a b E → ⋅ d l → = φ ( b → ) − φ ( a → ). ( displaystyle - int _ ( a ) ^ ( b ) ( ( \vec ( E ) ) cdot mathrm ( d ) ( \vec ( ell ) ) ) = phi ( ( \vec ( b ) ) ) - phi ( ( \vec ( a ) ) ). ) From these equations, we see that the electric potential is constant in any region for which the electric field vanishes ( such as occurs inside a conducting object ). Electrostatic energy Main articles : Electric potential energy and Energy density A single test particle 's potential energy, U E single ( displaystyle U_ ( mathrm ( E ) ) ^ ( \text ( single ) ) ), can be calculated from a line integral of the work, q n E → ⋅ d l → ( displaystyle q_ ( n ) ( \vec ( E ) ) cdot mathrm ( d ) ( \vec ( ell ) ) ). We integrate from a point at infinity, and assume a collection of N ( displaystyle N ) particles of charge Q n ( displaystyle Q_ ( n ) ), are already situated at the points r → i ( displaystyle ( \vec ( r ) ) _ ( i ) ). This potential energy ( in Joules ) is : U E single = q φ ( r → ) = q 4 π ε 0 ∑ i = 1 N Q i ∥ R → i ∥ ( displaystyle U_ ( mathrm ( E ) ) ^ ( \text ( single ) ) = q phi ( ( \vec ( r ) ) ) = ( \frac ( q ) ( 4 pi \varepsilon _ ( 0 ) ) ) sum _ ( i = 1 ) ^ ( N ) ( \frac ( Q_ ( i ) ) ( left ( mathcal ( ( \vec ( R ) ) _ ( i ) ) ) \right ) ) ) where R i → = r → − r → i ( displaystyle ( \vec ( mathcal ( R_ ( i ) ) ) ) = ( \vec ( r ) ) - ( \vec ( r ) ) _ ( i ) ) is the distance of each charge Q i ( displaystyle Q_ ( i ) ) from the test charge q ( displaystyle q ), which situated at the point r → ( displaystyle ( \vec ( r ) ) ), and φ ( r → ) ( displaystyle phi ( ( \vec ( r ) ) ) ) is the electric potential that would be at r → ( displaystyle ( \vec ( r ) ) ) if the test charge were not present. If only two charges are present, the potential energy is k e Q 1 Q 2 / r ( displaystyle k_ ( e ) Q_ ( 1 ) Q_ ( 2 ) / r ). The total electric potential energy due a collection of N charges is calculating by assembling these particles one at a time : U E total = 1 4 π ε 0 ∑ j = 1 N Q j ∑ i = 1 j − 1 Q i r i j = 1 2 ∑ i = 1 N Q i φ i, ( displaystyle U_ ( mathrm ( E ) ) ^ ( \text ( total ) ) = ( \frac ( 1 ) ( 4 pi \varepsilon _ ( 0 ) ) ) sum _ ( j = 1 ) ^ ( N ) Q_ ( j ) sum _ ( i = 1 ) ^ ( j - 1 ) ( \frac ( Q_ ( i ) ) ( r_ ( ij ) ) ) = ( \frac ( 1 ) ( 2 ) ) sum _ ( i = 1 ) ^ ( N ) Q_ ( i ) phi _ ( i ), ) where the following sum from, j = 1 to N, excludes i = j : φ i = 1 4 π ε 0 ∑ j = 1 ( j ≠ i ) N Q j r i j. ( displaystyle phi _ ( i ) = ( \frac ( 1 ) ( 4 pi \varepsilon _ ( 0 ) ) ) sum _ ( j = 1 ( j \neq i ) ) ^ ( N ) ( \frac ( Q_ ( j ) ) ( r_ ( ij ) ) ). ) This electric potential, φ i ( displaystyle phi _ ( i ) ) is what would be measured at r → i ( displaystyle ( \vec ( r ) ) _ ( i ) ) if the charge Q i ( displaystyle Q_ ( i ) ) were missing. This formula obviously excludes the ( infinite ) energy that would be required to assemble each point charge from a disperse cloud of charge. The sum over charges can be converted into an integral over charge density using the prescription ∑ ( ⋯ ) → ∫ ( ⋯ ) ρ d 3 r ( displaystyle sum ( cdots ) \rightarrow int ( cdots ) \rho mathrm ( d ) ^ ( 3 ) r ) : U E total = 1 2 ∫ ρ ( r → ) φ ( r → ) d 3 ⁡ r = ε 0 2 ∫ E 2 d 3 ⁡ r ( displaystyle U_ ( mathrm ( E ) ) ^ ( \text ( total ) ) = ( \frac ( 1 ) ( 2 ) ) int \rho ( ( \vec ( r ) ) ) phi ( ( \vec ( r ) ) ) operatorname ( d ) ^ ( 3 ) r = ( \frac ( \varepsilon _ ( 0 ) ) ( 2 ) ) int left ( mathbf ( E ) ) \right ^ ( 2 ) operatorname ( d ) ^ ( 3 ) r ), This second expression for electrostatic energy uses the fact that the electric field is the negative gradient of the electric potential, as well as vector calculus identities in a way that resembles integration by parts. These two integrals for electric field energy seem to indicate two mutually exclusive formulas for electrostatic energy density, namely 1 2 ρ φ ( displaystyle ( \frac ( 1 ) ( 2 ) ) \rho phi ) and ε 0 2 E 2 ( displaystyle ( \frac ( \varepsilon _ ( 0 ) ) ( 2 ) ) E ^ ( 2 ) ) ; they yield equal values for the total electrostatic energy only if both are integrated over all space. Electrostatic pressure On a conductor, a surface charge will experience a force in the presence of an electric field. This force is the average of the discontinuous electric field at the surface charge. This average in terms of the field just outside the surface amounts to : P = ε 0 2 E 2 ( displaystyle P = ( \frac ( \varepsilon _ ( 0 ) ) ( 2 ) ) E ^ ( 2 ) ), This pressure tends to draw the conductor into the field, regardless of the sign of the surface charge. Triboelectric series Main article : Triboelectric effect The triboelectric effect is a type of contact electrification in which certain materials become electrically charged when they are brought into contact with a different material and then separated. One of the materials acquires a positive charge, and the other acquires an equal negative charge. The polarity and strength of the charges produced differ according to the materials, surface roughness, temperature, strain, and other properties. Amber, for example, can acquire an electric charge by friction with a material like wool. This property, first recorded by Thales of Miletus, was the first electrical phenomenon investigated by humans. Other examples of materials that can acquire a significant charge when rubbed together include glass rubbed with silk, and hard rubber rubbed with fur. Electrostatic generators Main article : Electrostatic generator The presence of surface charge imbalance means that the objects will exhibit attractive or repulsive forces. This surface charge imbalance, which yields static electricity, can be generated by touching two differing surfaces together and then separating them due to the phenomena of contact electrification and the triboelectric effect. Rubbing two nonconductive objects generates a great amount of static electricity. This is not just the result of friction ; two nonconductive surfaces can become charged by just being placed one on top of the other. Since most surfaces have a rough texture, it takes longer to achieve charging through contact than through rubbing. Rubbing objects together increases amount of adhesive contact between the two surfaces. Usually insulators, e.g., substances that do not conduct electricity, are good at both generating, and holding, a surface charge. Some examples of these substances are rubber, plastic, glass, and pith. Conductive objects only rarely generate charge imbalance except, for example, when a metal surface is impacted by solid or liquid nonconductors. The charge that is transferred during contact electrification is stored on the surface of each object. Static electric generators, devices which produce very high voltage at very low current and used for classroom physics demonstrations, rely on this effect. Note that the presence of electric current does not detract from the electrostatic forces nor from the sparking, from the corona discharge, or other phenomena. Both phenomena can exist simultaneously in the same system. See also : Friction machines, Wimshurst machines, and Van de Graaff generators. Charge neutralization Natural electrostatic phenomena are most familiar as an occasional annoyance in seasons of low humidity, but can be destructive and harmful in some situations ( e.g. electronics manufacturing ). When working in direct contact with integrated circuit electronics ( especially delicate MOSFETs ), or in the presence of flammable gas, care must be taken to avoid accumulating and suddenly discharging a static charge ( see electrostatic discharge ). Electrostatic induction Main article : Electrostatic induction Electrostatic induction, discovered by British scientist John Canton in 1753 and Swedish professor Johan Carl Wilcke in 1762 is a redistribution of charges in an object caused by the electric field of a nearby charge. For example, if a positively charged object is brought near an uncharged metal object, the mobile negatively - charged electrons in the metal will be attracted the external charge, and move to the side of the metal facing it, creating a negative charge on the surface. When the electrons move out of an area they leave a positive charge due to the metal atoms ' nuclei, so the side of the metal object facing away from the charge acquires a positive charge. These induced charges disappear when the external charge is removed. Induction is also responsible for the attraction of light objects, such as balloons, paper scraps and styrofoam packing peanuts to static charges. The surface charges induced in conductive objects exactly cancel external electric fields inside the conductor, so there is no electric field inside a metal object. This is the basis for the electric field shielding action of a Faraday cage. Since the electric field is the gradient of the voltage, electrostatic induction is also responsible for making the electric potential ( voltage ) constant throughout a conductive object. ' Static ' electricity Main article : Static electricity Lightning over Oradea in Romania Before the year 1832, when Michael Faraday published the results of his experiment on the identity of electricities, physicists thought `` static electricity '' was somehow different from other electrical charges. Michael Faraday proved that the electricity induced from the magnet, voltaic electricity produced by a battery, and static electricity are all the same. Static electricity is usually caused when certain materials are rubbed against each other, like wool on plastic or the soles of shoes on carpet. The process causes electrons to be pulled from the surface of one material and relocated on the surface of the other material. A static shock occurs when the surface of the second material, negatively charged with electrons, touches a positively charged conductor, or vice versa. Static electricity is commonly used in xerography, air filters, and some automotive paints. Static electricity is a buildup of electric charges on two objects that have become separated from each other. Small electrical components can easily be damaged by static electricity. Component manufacturers use a number of antistatic devices to avoid this. Static electricity and chemical industry When different materials are brought together and then separated, an accumulation of electric charge can occur which leaves one material positively charged while the other becomes negatively charged. The mild shock that you receive when touching a grounded object after walking on carpet is an example of excess electrical charge accumulating in your body from frictional charging between your shoes and the carpet. The resulting charge build - up upon your body can generate a strong electrical discharge. Although experimenting with static electricity may be fun, similar sparks create severe hazards in those industries dealing with flammable substances, where a small electrical spark may ignite explosive mixtures with devastating consequences. A similar charging mechanism can occur within low conductivity fluids flowing through pipelines -- a process called flow electrification. Fluids which have low electrical conductivity ( below 50 picosiemens per meter ), are called accumulators. Fluids having conductivities above 50 pS / m are called non-accumulators. In non-accumulators, charges recombine as fast as they are separated and hence electrostatic charge generation is not significant. In the petrochemical industry, 50 pS / m is the recommended minimum value of electrical conductivity for adequate removal of charge from a fluid. An important concept for insulating fluids is the static relaxation time. This is similar to the time constant ( tau ) within an RC circuit. For insulating materials, it is the ratio of the static dielectric constant divided by the electrical conductivity of the material. For hydrocarbon fluids, this is sometimes approximated by dividing the number 18 by the electrical conductivity of the fluid. Thus a fluid that has an electrical conductivity of 1 pS / cm ( 100 pS / m ) will have an estimated relaxation time of about 18 seconds. The excess charge within a fluid will be almost completely dissipated after 4 to 5 times the relaxation time, or 90 seconds for the fluid in the above example. Charge generation increases at higher fluid velocities and larger pipe diameters, becoming quite significant in pipes 8 inches ( 200 mm ) or larger. Static charge generation in these systems is best controlled by limiting fluid velocity. The British standard BS PD CLC / TR 50404 : 2003 ( formerly BS - 5958 - Part 2 ) Code of Practice for Control of Undesirable Static Electricity prescribes velocity limits. Because of its large impact on dielectric constant, the recommended velocity for hydrocarbon fluids containing water should be limited to 1 m / s. Bonding and earthing are the usual ways by which charge buildup can be prevented. For fluids with electrical conductivity below 10 pS / m, bonding and earthing are not adequate for charge dissipation, and anti-static additives may be required. Applicable standards 1.BS PD CLC / TR 50404 : 2003 Code of Practice for Control of Undesirable Static Electricity 2. NFPA 77 ( 2007 ) Recommended Practice on Static Electricity 3. API RP 2003 ( 1998 ) Protection Against Ignitions Arising Out of Static, Lightning, and Stray Currents Electrostatic induction in commercial applications Electrostatic induction was used in the past to build high - voltage generators known as Influence machines. The main component that emerged in these times is the capacitor. Electrostatic induction is also used for electro - mechanic precipitation or projection.In such technologies, charged particles of small sizes are collected or deposited intentionally on surfaces. Applications range from Electrostatic precipitator to Spray painting or Inkjet printing. Recently a new Wireless power Transfer Technology has been based on electrostatic induction between oscillating distant dipoles. See also Electromagnetism Permittivity and relative permittivity Ionic bond Electronegativity Electrostatic discharge Electrostatic separator Electrostatic voltmeter Quantisation Of Charge References Faraday, Michael ( 1839 ). Experimental Researches in Electricity. London : Royal Inst. e-book at Project Gutenberg Halliday, David ; Robert Resnick ; Kenneth S. Krane ( 1992 ). Physics. New York : John Wiley & Sons. ISBN 0 - 471 - 80457 - 6. Griffiths, David J. ( 1999 ). Introduction to Electrodynamics. Upper Saddle River, NJ : Prentice Hall. ISBN 0 - 13 - 805326 - X. Hermann A. Haus ; James R. Melcher ( 1989 ). Electromagnetic Fields and Energy. Englewood Cliffs, NJ : Prentice - Hall. ISBN 0 - 13 - 249020 - X. Jump up ^ Matthew Sadiku ( 2009 ). Elements of electromagnetics. p. 104. ISBN 9780195387759. ^ Jump up to : Purcell, Edward M. ( 2013 ). Electricity and Magnetism. Cambridge University Press. pp. 16 -- 18. ISBN 1107014026. Jump up ^ Heras, J.A. ( 2010 ). `` The Galilean limits of Maxwell 's equations ''. American Journal of Physics. 78 ( 10 ) : 1048. arXiv : 1012.1068. Bibcode : 2010AmJPh... 78.1048 H. doi : 10.1119 / 1.3442798. Jump up ^ `` Electricity ''. Encyclopaedia Britannica, 11th Ed. 9. The Encyclopaedia Britannica Co. 1910. p. 181. Retrieved 2008 - 06 - 23. Jump up ^ Heilbron, J.L. ( 1979 ). Electricity in the 17th and 18th Centuries : A Study of Early Modern Physics. Univ. of California Press. ISBN 0520034783. Jump up ^ Sarkar, T.K. ; Mailloux, Robert ; Oliner, Arthur A., Ed. ( 2006 ). History of Wireless. John Wiley and Sons. p. 9. ISBN 0471783013. Further reading Essays William J. Beaty, `` Humans and sparks ; The Cause, Stopping the Pain, and ' Electric People ''. 1997. Books William Cecil Dampier, `` The theory of experimental electricity ''. Cambridge ( Eng. ) University press, 1905 ( Cambridge physical series ). xi, 334 p. illus., diagrs. 23 cm. LCCN 05040419 / / r33 William Thomson Kelvin, Reprint of Papers on Electrostatics and Magnetism By William Thomson Kelvin, Macmillan 1872 Alexander MacAulay Utility of Quaternions in Physics. Electrostatics -- General Problem. Macmillan 1893 Alexander Russell, A Treatise on the Theory of Alternating Currents. Electrostatics. University Press 1904 External links Look up electrostatics in Wiktionary, the free dictionary. Man 's static jacket sparks alert ``. BBC News, 16 September 2005. Static Electricity and Plastics `` Can shocks from static electricity damage your health ? ''. Wolfson Electrostatics News pages. Invisible wall of static : Downloadable electrostatic BEM modules in MATLAB for simple capacitance problems Introduction to Electrostatics : Point charges can be treated as a distribution using the Dirac delta function Library resources about Electrostatics Resources in your library Learning materials related to Electrostatics at Wikiversity GND : 4151975 - 9 Retrieved from `` https://en.wikipedia.org/w/index.php?title=Electrostatics&oldid=814428228 '' Categories : Concepts in physics Electrostatics Hidden categories : Articles containing Ancient Greek - language text All pages needing factual verification Wikipedia articles needing factual verification from May 2016 Articles with Project Gutenberg links Wikipedia articles with GND identifiers Talk Contents About Wikipedia Wikibooks Alemannisch Azərbaycanca Беларуская Беларуская ( тарашкевіца ) ‎ Български Bosanski Català Čeština Dansk Deutsch Eesti Ελληνικά Español Esperanto Euskara فارسی Français Gaeilge Galego 한국어 Հայերեն हिन्दी Hrvatski Ido Bahasa Indonesia Italiano עברית ქართული Қазақша Latviešu Lietuvių Magyar Македонски മലയാളം Nederlands 日本 語 Nordfriisk Norsk Norsk nynorsk ਪੰਜਾਬੀ پنجابی Piemontèis Polski Português Română Русский Scots Shqip Simple English Slovenčina Slovenščina Српски / srpski Srpskohrvatski / српскохрватски Basa Sunda Suomi Svenska தமிழ் Татарча / tatarça తెలుగు ไทย Türkçe Українська اردو Tiếng Việt Wolof 粵語 中文 Edit links This page was last edited on 8 December 2017, at 19 : 48. 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Question: what is the area in physics that deals with stationary electrical charges
Answer: Electrostatics