Electrostatics

Electrostatics is a branch of that studies s at rest.

Since, it has been known that some materials such as  attract lightweight particles after. The word for amber, ??e?t???, or electron, was the source of the word 'electricity'. Electrostatic phenomena arise from the s that electric charges exert on each other. Such forces are described by. Even though electrostatically induced forces seem to be rather weak, some electrostatic forces such as the one between an and a, that together make up a  , is about 36  stronger than the al force acting between them.

There are many examples of electrostatic phenomena, from those as simple as the attraction of the plastic wrap to one's hand after it is removed from a package to the apparently spontaneous explosion of grain silos, the damage of electronic components during manufacturing, and &  operation. Electrostatics involves the buildup of charge on the 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 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 : 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.

Coulomb's law
Coulomb's law states that:

'The magnitude of the electrostatic force of attraction or repulsion between two point charges is directly proportional to the product of the magnitudes of charges and inversely proportional to the square of the distance between them.'

The force is along the straight line joining them. If the two charges have the same sign, the electrostatic force between them is repulsive; if they have different signs, the force between them is attractive.

If $$r$$ is the distance (in ) between two charges, then the force (in s) between two point charges $$q$$ and $$Q$$ (in s) is:


 * $$F = \frac{1}{4\pi \varepsilon_0}\frac{qQ}{r^2}= k_0\frac{qQ}{r^2}\, ,$$

where e0 is the, or permittivity of free space:


 * $$\varepsilon_0 \approx {10^{-9}\over 36\pi} \;\; \mathrm{C^2\ N^{-1}\ m^{-2}}\approx 8.854\ 187\ 817 \times 10^{-12} \;\; \mathrm{C^2\ N^{-1}\ m^{-2}}. $$

The units of e0 are equivalently &ensp;24 kg-1m-3 or 2&minus;1m&minus;2 or  m&minus;1. is:


 * $$ k_0 = \frac{1}{4\pi\varepsilon_0}\approx 8.987\ 551\ 787 \times 10^9 \;\; \mathrm{N\ m^2\ C}^{-2}. $$

A single has a charge of e, and the  has a charge of -e, where,


 * $$ e \approx 1.602\ 176\ 565 \times 10^{-19}\;\; \mathrm{C}. $$

These s (e0, k0, e) are currently defined so that e0 and k0 are exactly defined, and e is a measured quantity.

Electric field
The, $$\vec{E}$$, in units of per  or s per meter, is a  that can be defined everywhere, except at the location of point charges (where it diverges to infinity). It is defined as the electrostatic force $$\vec{F}\,$$ in newtons on a hypothetical small at the point due to, divided by the magnitude of the charge $$q\,$$ in coulombs


 * $$\vec{E} = {\vec{F} \over q}\,$$

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 $$N$$ particles of charge $$Q_i$$, located at points $$\vec r_i$$ (called source points), the electric field at $$\vec r $$ (called the field point) is:


 * $$ \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 $$ \vec\mathcal R_i =  \vec r - \vec r_i ,$$ is the displacement vector from a source point $$\vec r_i$$ to the field point $$\vec r $$, and $$ \widehat\mathcal R_i = \vec\mathcal R_i / \left \|\vec\mathcal R_i \right \|$$ is a that indicates the direction of the field. For a single point charge at the origin, the magnitude of this electric field is $$E =k_eQ/\mathcal R^2,$$ 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. The electric field produced by a distribution of charges is given by the volume $$\rho (\vec r)$$ and can be obtained by converting this sum into a :


 * $$\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' 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 enclosed by the surface." Mathematically, Gauss's law takes the form of an integral equation:


 * $$\oint_S\vec{E} \cdot\mathrm{d}\vec{A} = \frac{1}{\varepsilon_0}\,Q_{enclosed}=\int_V{\rho\over\varepsilon_0}\cdot\operatorname{d}^3 r,$$

where $$ \operatorname{d}^3 r =\mathrm{d}x \ \mathrm{d}y \ \mathrm{d}z $$ is a volume element. If the charge is distributed over a surface or along a line, replace $$ \rho\mathrm{d}^3r $$ by $$ \sigma\mathrm{d}A $$ or $$ \lambda\mathrm{d}\ell $$. The allows Gauss's Law to be written in differential form:


 * $$\vec{\nabla}\cdot\vec{E} = {\rho\over\varepsilon_0}.$$

where $$\vec{\nabla} \cdot$$ is the.

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 F and the charge density ?:


 * $${\nabla}^2 \phi = - {\rho\over\varepsilon_0}.$$

This relationship is a form of. In the absence of unpaired electric charge, the equation becomes :


 * $${\nabla}^2 \phi = 0,$$

Electrostatic approximation
The validity of the electrostatic approximation rests on the assumption that the electric field is :


 * $$\vec{\nabla}\times\vec{E} = 0.$$

From, this assumption implies the absence or near-absence of time-varying magnetic fields:


 * $${\partial\vec{B}\over\partial t} = 0.$$

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 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, it is possible to express the electric field as the of a scalar function,$$\phi$$, called the  (also known as the ). An electric field, $$E$$, points from regions of high electric potential to regions of low electric potential, expressed mathematically as


 * $$\vec{E} = -\vec{\nabla}\phi.$$

The can be used to establish that the electrostatic potential is the amount of  per unit charge required to move a charge from point $$a$$ to point $$b$$ with the following :


 * $$ -\int_a^b{\vec{E}\cdot \mathrm{d}\vec \ell} = \phi (\vec b) -\phi(\vec a).$$

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
A single 's potential energy, $$ U_\mathrm{E}^{\text{single}}$$, can be calculated from a  of the work, $$q_n\vec E\cdot\mathrm d\vec\ell $$. We integrate from a point at infinity, and assume a collection of $$N$$ particles of charge $$Q_n$$, are already situated at the points $$\vec r_i$$. This potential energy (in s) is:


 * $$ U_\mathrm{E}^{\text{single}}=q\phi(\vec r)=\frac{q }{4\pi \varepsilon_0}\sum_{i=1}^N \frac{Q_i}{\left \|\mathcal{\vec R_i} \right \|} $$

where $$ \vec\mathcal {R_i} = \vec r - \vec r_i$$ is the distance of each charge $$Q_i$$ from the  $$q$$, which situated at the point $$\vec r $$, and $$ \phi(\vec r)$$  is the electric potential that would be at $$\vec r $$ if the  were not present. If only two charges are present, the potential energy is $$k_eQ_1Q_2/r$$. The total due a collection of N charges is calculating by assembling these particles :


 * $$U_\mathrm{E}^{\text{total}} = \frac{1 }{4\pi \varepsilon _0}\sum_{j=1}^N Q_j \sum_{i=1}^{j-1} \frac{Q_i}{r_{ij}}= \frac{1}{2}\sum_{i=1}^N Q_i\phi_i ,$$

where the following sum from, j = 1 to N, excludes i = j:


 * $$\phi_i = \frac{1}{4\pi \varepsilon _0}\sum_{j=1 (j\ne i)}^N \frac{Q_j}{r_{ij}}. $$

This electric potential, $$\phi_i$$ is what would be measured at $$\vec r_i$$ if the charge $$Q_i$$ 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 $$\sum (\cdots) \rightarrow \int(\cdots)\rho\mathrm d^3r$$:


 * $$U_\mathrm{E}^{\text{total}} = \frac{1}{2} \int\rho(\vec{r})\phi(\vec{r}) \operatorname{d}^3 r = \frac{\varepsilon_0 }{2} \int \left|{\mathbf{E}}\right|^2 \operatorname{d}^3 r$$,

This second expression for uses the fact that the electric field is the negative  of the electric potential, as well as  in a way that resembles. These two integrals for electric field energy seem to indicate two mutually exclusive formulas for electrostatic energy density, namely $$\frac{1}{2}\rho\phi$$ and $$\frac{\varepsilon_0 }{2}E^2$$; they yield equal values for the total electrostatic energy only if both are integrated over all space.

Electrostatic pressure
On a, a surface charge will experience a force in the presence of an. 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:


 * $$ P = \frac{ \varepsilon_0 }{2} E^2 $$,

This pressure tends to draw the conductor into the field, regardless of the sign of the surface charge.

Triboelectric series
The 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, 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
The presence of 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 and the. 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, e.g., substances that do not conduct electricity, are good at both generating, and holding, a surface charge. Some examples of these substances are, , , and. 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. , 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 does not detract from the electrostatic forces nor from the sparking, from the, or other phenomena. Both phenomena can exist simultaneously in the same system.


 * See also: s, s, and s.

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 s), or in the presence of flammable gas, care must be taken to avoid accumulating and suddenly discharging a static charge (see ).

Electrostatic induction
Electrostatic induction, discovered by British scientist in 1753 and Swedish professor  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 s 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', 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. Since the electric field is the of the voltage, electrostatic induction is also responsible for making the   constant throughout a conductive object.

'Static' electricity
Before the year 1832, when 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, s, 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 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, 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. For insulating materials, it is the ratio of the static 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 in 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 s. The main component that emerged in these times is the. 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 to  or. Recently a new Transfer Technology has been based on electrostatic induction between oscillating distant dipoles.