Electric current

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Electric current
SI unit
ampere
Derivations from
other quantities
Dimension

An electric current is a flow of

electric circuits the charge carriers are often electrons moving through a wire. In semiconductors they can be electrons or holes. In an electrolyte the charge carriers are ions, while in plasma, an ionized gas, they are ions and electrons.[6]

In the

base quantity in the International System of Quantities (ISQ).[7]: 15  Electric current is also known as amperage and is measured using a device called an ammeter.[5]
: 788 

Electric currents create

electromagnetic waves, which are used in telecommunications to broadcast information.[10]

Symbol

The conventional symbol for current is I, which originates from the French phrase intensité du courant, (current intensity).[11][12] Current intensity is often referred to simply as current.[13] The I symbol was used by André-Marie Ampère, after whom the unit of electric current is named, in formulating Ampère's force law (1820).[14] The notation travelled from France to Great Britain, where it became standard, although at least one journal did not change from using C to I until 1896.[15]

Conventions

The electrons, the charge carriers in an electrical circuit, flow in the opposite direction of the conventional electric current.
The symbol for a battery in a circuit diagram.

The conventional direction of current, also known as conventional current,

electrical circuits, the positively charged atomic nuclei of the atoms are held in a fixed position, and the negatively charged electrons are the charge carriers, free to move about in the metal. In other materials, notably the semiconductors, the charge carriers can be positive or negative, depending on the dopant used. Positive and negative charge carriers may even be present at the same time, as happens in an electrolyte in an electrochemical cell
.

A flow of positive charges gives the same electric current, and has the same effect in a circuit, as an equal flow of negative charges in the opposite direction. Since current can be the flow of either positive or negative charges, or both, a convention is needed for the direction of current that is independent of the type of charge carriers. Negatively charged carriers, such as the electrons (the charge carriers in metal wires and many other electronic circuit components), therefore flow in the opposite direction of conventional current flow in an electrical circuit.[16][17]

Reference direction

A current in a wire or

circuit element can flow in either of two directions. When defining a variable
to represent the current, the direction representing positive current must be specified, usually by an arrow on the : 13  This is called the reference direction of the current . When
analyzing electrical circuits, the actual direction of current through a specific circuit element is usually unknown until the analysis is completed. Consequently, the reference directions of currents are often assigned arbitrarily. When the circuit is solved, a negative value for the current implies the actual direction of current through that circuit element is opposite that of the chosen reference direction.[a]
: 29 

Ohm's law

Ohm's law states that the current through a conductor between two points is directly

resistance,[20] one arrives at the usual mathematical equation that describes this relationship:[21]

where I is the current through the conductor in units of

resistance of the conductor in units of ohms. More specifically, Ohm's law states that the R in this relation is constant, independent of the current.[22]

Alternating and direct current

In

modulated
) onto the AC signal.

In contrast,

electron or ion beams. An old name for direct current was galvanic current.[24]

Occurrences

Natural observable examples of electric current include

]

Man-made occurrences of electric current include the controlled flow of conduction electrons in metal wires, such as overhead power lines for long-distance energy delivery and the smaller wires within electrical and electronic devices.[

are generated.

In

battery, and the flow of holes within metals and semiconductors
.

A biological example of current is the flow of ions in

neurons
and nerves, responsible for both thought and sensory perception.

Measurement

Current can be measured using an

techniques
to measure current:

Resistive heating

Joule heating, also known as ohmic heating and resistive heating, is the process of

electrical resistance
of the wire.

This relationship is known as

SI unit of energy was subsequently named the joule and given the symbol J.[7]: 20  The commonly known SI unit of power, the watt (symbol: W), is equivalent to one joule per second.[7]
: 20 

Electromagnetism

Electromagnet

Magnetic field is produced by an electric current in a solenoid.

In an electromagnet a coil of wires behaves like a magnet when an electric current flows through it.[33][34] When the current is switched off, the coil loses its magnetism immediately. Electric current produces a magnetic field.[35] The magnetic field can be visualized as a pattern of circular field lines surrounding the wire that persists as long as there is current.

Electromagnetic induction

Alternating electric current flows through the solenoid, producing a changing magnetic field. This field causes an electric current to flow in the wire loop by electromagnetic induction.

Magnetic fields can also be used to make electric currents. When a changing magnetic field is applied to a conductor, an electromotive force (EMF) is induced,[32]: 1004  which starts an electric current, when there is a suitable path.

Radio waves

When an electric current flows in a

radio waves can be generated. These travel at the speed of light
and can cause electric currents in distant conductors.

Conduction mechanisms in various media

In metallic solids, electric charge flows by means of

electrical potential
. In other media, any stream of charged objects (ions, for example) may constitute an electric current. To provide a definition of current independent of the type of charge carriers, conventional current is defined as moving in the same direction as the positive charge flow. So, in metals where the charge carriers (electrons) are negative, conventional current is in the opposite direction to the overall electron movement. In conductors where the charge carriers are positive, conventional current is in the same direction as the charge carriers.

In a

plasma
are flows of electrons as well as positive and negative ions. In ice and in certain solid electrolytes, the electric current is entirely composed of flowing ions.

Metals

In a

One, Two, Three...Infinity
(1947), "The metallic substances differ from all other materials by the fact that the outer shells of their atoms are bound rather loosely, and often let one of their electrons go free. Thus the interior of a metal is filled up with a large number of unattached electrons that travel aimlessly around like a crowd of displaced persons. When a metal wire is subjected to electric force applied on its opposite ends, these free electrons rush in the direction of the force, thus forming what we call an electric current."

When a metal wire is connected across the two terminals of a

positive terminal under the influence of this field. The free electrons are therefore the charge carrier
in a typical solid conductor.

For a steady flow of charge through a surface, the current I (in amperes) can be calculated with the following equation:

where Q is the electric charge transferred through the surface over a
time t. If Q and t are measured in coulombs and seconds respectively, I is in amperes.

More generally, electric current can be represented as the rate at which charge flows through a given surface as:

Electrolytes

A proton conductor in a static electric field.

Electric currents in electrolytes are flows of electrically charged particles (ions). For example, if an electric field is placed across a solution of Na+ and Cl (and conditions are right) the sodium ions move towards the negative electrode (cathode), while the chloride ions move towards the positive electrode (anode). Reactions take place at both electrode surfaces, neutralizing each ion.

Water-ice and certain solid electrolytes called proton conductors contain positive hydrogen ions ("protons") that are mobile. In these materials, electric currents are composed of moving protons, as opposed to the moving electrons in metals.

In certain electrolyte mixtures, brightly coloured ions are the moving electric charges. The slow progress of the colour makes the current visible.[37]

Gases and plasmas

In air and other ordinary

ionizing, neutral gas atoms or molecules in a process called avalanche breakdown. The breakdown process forms a plasma that contains enough mobile electrons and positive ions to make it an electrical conductor. In the process, it forms a light emitting conductive path, such as a spark, arc or lightning
.

Plasma is the state of matter where some of the electrons in a gas are stripped or "ionized" from their molecules or atoms. A plasma can be formed by high temperature, or by application of a high electric or alternating magnetic field as noted above. Due to their lower mass, the electrons in a plasma accelerate more quickly in response to an electric field than the heavier positive ions, and hence carry the bulk of the current. The free ions recombine to create new chemical compounds (for example, breaking atmospheric oxygen into single oxygen [O2 → 2O], which then recombine creating ozone [O3]).[38]

Vacuum

Since a "

filament or indirectly heated cathode of vacuum tubes. Cold electrodes can also spontaneously produce electron clouds via thermionic emission when small incandescent regions (called cathode spots or anode spots) are formed. These are incandescent regions of the electrode surface that are created by a localized high current. These regions may be initiated by field electron emission, but are then sustained by localized thermionic emission once a vacuum arc forms. These small electron-emitting regions can form quite rapidly, even explosively, on a metal surface subjected to a high electrical field. Vacuum tubes and sprytrons
are some of the electronic switching and amplifying devices based on vacuum conductivity.

Superconductivity

Superconductivity is a phenomenon of exactly zero

atomic spectral lines, superconductivity is a quantum mechanical phenomenon. It is characterized by the Meissner effect, the complete ejection of magnetic field lines from the interior of the superconductor as it transitions into the superconducting state. The occurrence of the Meissner effect indicates that superconductivity cannot be understood simply as the idealization of perfect conductivity in classical physics
.

Semiconductor

In a

insulator. This means a conductivity roughly in the range of 10−2 to 104 siemens
per centimeter (S⋅cm−1).

In the classic crystalline semiconductors, electrons can have energies only within certain bands (i.e. ranges of levels of energy). Energetically, these bands are located between the energy of the ground state, the state in which electrons are tightly bound to the atomic nuclei of the material, and the free electron energy, the latter describing the energy required for an electron to escape entirely from the material. The energy bands each correspond to many discrete

metals
because the valence band in any given metal is nearly filled with electrons under usual operating conditions, while very few (semiconductor) or virtually none (insulator) of them are available in the conduction band, the band immediately above the valence band.

The ease of exciting electrons in the semiconductor from the valence band to the conduction band depends on the

insulators
.

With covalent bonds, an electron moves by hopping to a neighboring bond. The

electrical conductivity. However, as a semiconductor's temperature rises above absolute zero
, there is more energy in the semiconductor to spend on lattice vibration and on exciting electrons into the conduction band. The current-carrying electrons in the conduction band are known as free electrons, though they are often simply called electrons if that is clear in context.

Current density and Ohm's law

Current density is the rate at which charge passes through a chosen unit area.

SI units, current density (symbol: j) is expressed in the SI base units of amperes per square metre.[7]
: 22 

In linear materials such as metals, and under low frequencies, the current density across the conductor surface is uniform. In such conditions,

ohmic device
):

where is the current, measured in amperes; is the

; and is the
resistance, measured in ohms. For alternating currents, especially at higher frequencies, skin effect
causes the current to spread unevenly across the conductor cross-section, with higher density near the surface, thus increasing the apparent resistance.

Drift speed

The mobile charged particles within a conductor move constantly in random directions, like the particles of a gas. (More accurately, a Fermi gas.) To create a net flow of charge, the particles must also move together with an average drift rate. Electrons are the charge carriers in most metals and they follow an erratic path, bouncing from atom to atom, but generally drifting in the opposite direction of the electric field. The speed they drift at can be calculated from the equation:

where

  • is the drift velocity
  • is the electric current
  • is number of charged particles per unit volume (or charge carrier density)
  • is the cross-sectional area of the conductor
  • is the charge on each particle.

Typically, electric charges in solids flow slowly. For example, in a copper wire of cross-section 0.5 mm2, carrying a current of 5 A, the drift velocity of the electrons is on the order of a millimetre per second. To take a different example, in the near-vacuum inside a cathode-ray tube, the electrons travel in near-straight lines at about a tenth of the speed of light.

Any accelerating electric charge, and therefore any changing electric current, gives rise to an

load
, even though the electrons in the wires only move back and forth over a tiny distance.

The ratio of the speed of the electromagnetic wave to the speed of light in free space is called the velocity factor, and depends on the electromagnetic properties of the conductor and the insulating materials surrounding it, and on their shape and size.

The magnitudes (not the natures) of these three velocities can be illustrated by an analogy with the three similar velocities associated with gases. (See also hydraulic analogy.)

  • The low drift velocity of charge carriers is analogous to air motion; in other words, winds.
  • The high speed of electromagnetic waves is roughly analogous to the speed of sound in a gas (sound waves move through air much faster than large-scale motions such as convection)
  • The random motion of charges is analogous to heat – the thermal velocity of randomly vibrating gas particles.

See also

Notes

  1. ^ Our first step in the analysis is the assumption of reference directions for the unknown currents.[19]

References

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  5. ^ .
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  7. ^
  8. .
  9. .
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  11. .
  12. .
  13. . 'Current intensity' is usually referred to as 'current' itself.
  14. ^ Ampère, A-M (1822). "Recueil d'Observations Électro-dynamiques" (PDF) (in French). Paris: Chez Crochard Libraire. p. 56. Archived (PDF) from the original on 2011-07-24.
  15. ^ Electric Power. Vol. 6. 1894. pp. 411, 1894.
  16. ^ .
  17. ^ .
  18. .
  19. ^ .
  20. ^ Consoliver, Earl L.; Mitchell, Grover I. (1920). Automotive ignition systems. McGraw-Hill. p. 4. ohm's law current proportional voltage resistance.
  21. Robert A. Millikan and E. S. Bishop (1917). Elements of Electricity. American Technical Society. p. 54
    . Ohm's law current directly proportional.
  22. .
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  28. .
  29. ^ "What is a Current Sensor and How is it Used?". Retrieved 2011-12-22.
  30. ^ Friedrich, Andreas P.; Lemme, Helmuth (2000-05-01). "The Universal Current Sensor". Fierce Electronics. Archived from the original on 2016-03-04. Retrieved 2011-12-22.
  31. ^ a b Jaffe, Robert L.; Taylor, Washington (2018). The physics of energy. Cambridge University Press.
  32. ^ .
  33. .
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  35. .
  36. ^ "The Mechanism Of Conduction In Metals". Think Quest. Archived from the original on 2012-10-25.
  37. .
  38. ^ "Lab Note #106 Environmental Impact of Arc Suppression". Arc Suppression Technologies. April 2011. Retrieved March 15, 2012.
  39. .