Electric Field

Electric field

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In physics, the space surrounding an electric charge or in the presence of a time-varying magnetic field has a property called an electric field. This electric field exerts a force on other electrically charged objects. The concept of an electric field was introduced by Michael Faraday.

The electric field is a vector field with SI units of newtons per coulomb (N C⁻¹) or, equivalently, volts per metre (V m⁻¹). The SI base units of the electric field are kg·m·s⁻³·A⁻¹. The strength of the field at a given point is defined as the force that would be exerted on a positive test charge of +1 coulomb placed at that point; the direction of the field is given by the direction of that force. Electric fields contain electrical energy with energy density proportional to the square of the field intensity. The electric field is to charge as gravitational acceleration is to mass and force density is to volume.

A moving charge has not just an electric field but also a magnetic field, and in general the electric and magnetic fields are not completely separate phenomena; what one observer perceives as an electric field, another observer in a different frame of reference perceives as a mixture of electric and magnetic fields. For this reason, one speaks of "electromagnetism" or "electromagnetic fields." In quantum mechanics, disturbances in the electromagnetic fields are called photons, and the energy of photons is quantized.

[edit] Definition

A stationary charged particle in an electric field experiences a force proportional to its charge given by the equation

where the magnetic flux density is given by

and where is the Coulomb force. (See the section below).

Electric charge is a characteristic of some subatomic particles, determining how they interact electromagnetically. Stable independent objects carry charge in integer multiples of the so-called elementary charge e. Electrons by convention have a charge of −1, while protons have the opposite charge of +1.

In general, same-sign charged particles repel one another, while different-sign charged particles attract. This is expressed quantitatively in Coulomb's law, which states the magnitude of the repelling force is proportional to the product of the two charges, and weakens proportionately to the square of the distance.

The electric charge of a macroscopic object is the sum of the electric charges of its constituent particles. Often, the net electric charge is zero, since naturally the number of electrons in every atom is equal to the number of the protons, so their charges cancel out. Situations in which the net charge is non-zero are often referred to as static electricity. Furthermore, even when the net charge is zero, it can be distributed non-uniformly (e.g., due to an external electric field), and then the material is said to be polarized, and the charge related to the polarization is known as bound charge (while the excess charge brought from outside is called free charge). An ordered motion of charged particles in a particular direction (in metals, these are the electrons) is known as electric current. The discrete nature of electric charge was proposed by Michael Faraday in his electrolysis experiments, then directly demonstrated by Robert Millikan in his oil-drop experiment.

The SI unit for quantity of electricity or electric charge is the coulomb, which represents approximately 6.25 × 10¹⁸ elementary charges (the charge on a single electron or proton). The coulomb is defined as the quantity of charge that has passed through the cross-section of an electrical conductor carrying one ampere within one second. The symbol Q is often used to denote a quantity of electricity or charge. The quantity of electric charge can be directly measured with an electrometer, or indirectly measured with a ballistic galvanometer.

Formally, a measure of charge should be a multiple of the elementary charge e (charge is quantized), but since it is an average, macroscopic quantity, many orders of magnitude larger than a single elementary charge, it can effectively take on any real value. Furthermore, in some contexts it is meaningful to speak of fractions of a charge; e.g. in the charging of a capacitor.

If the charged particle can be considered a point charge, the electric field is defined as the force it experiences per unit charge:

where

is the electric force experienced by the particle

q is its charge

is the electric field wherein the particle is located

Taken literally, this equation only defines the electric field at the places where there are stationary charges present to experience it. Furthermore, the force exerted by another charge q will alter the source distribution, which means the electric field in the presence of q differs from itself in the absence of q. However, the electric field of a given source distribution remains defined in the absence of any charges with which to interact. This is achieved by measuring the force exerted on successively smaller test charges placed in the vicinity of the source distribution. By this process, the electric field created by a given source distribution is defined as the limit as the test charge approaches zero of the force per unit charge exerted thereupon.

This allows the electric field to be dependent on the source distribution alone.

As is clear from the definition, the direction of the electric field is the same as the direction of the force it would exert on a positively-charged particle, and opposite the direction of the force on a negatively-charged particle. Since like charges repel and opposites attract (as quantified below), the electric field tends to point away from positive charges and towards negative charges.

[edit] Coulomb's law

The electric field surrounding a point charge is given by Coulomb's law:

where

Q is the charge of the particle creating the electric force,

r is the distance from the particle with charge Q to the E-field evaluation point,

is the unit vector pointing from the particle with charge Q to the E-field evaluation point,

is the electric constant.

Coulomb's law is actually a special case of Gauss's Law, a more fundamental description of the relationship between the distribution of electric charge in space and the resulting electric field. Gauss's law is one of Maxwell's equations, a set of four laws governing electromagnetics.

[edit] Time-varying fields

Charges do not only produce electric fields. As they move, they generate magnetic fields, and if the magnetic field changes, it generates electric fields. A changing magnetic field gives rise to an electric field,

which yields Faraday's law of induction,

where

indicates the curl of the electric field,

represents the vector rate of decrease of magnetic field with time.

This means that a magnetic field changing in time produces a curled electric field, possibly also changing in time. The situation in which electric or magnetic fields change in time is no longer electrostatics, but rather electrodynamics or electromagnetics.

[edit] Properties (in electrostatics)

Illustration of the electric field surrounding a positive (red) and a negative (green) charge.

According to equation (1) above, electric field is dependent on position. The electric field due to any single charge falls off as the square of the distance from that charge.

Electric fields follow the superposition principle. If more than one charge is present, the total electric field at any point is equal to the vector sum of the respective electric fields that each object would create in the absence of the others.

If this principle is extended to an infinite number of infinitesimally small elements of charge, the following formula results:

where

ρ is the charge density, or the amount of charge per unit volume.

The electric field at a point is equal to the negative gradient of the electric potential there. In symbols,

where

φ(x,y,z) is the scalar field representing the electric potential at a given point.

If several spatially distributed charges generate such an electric potential, e.g. in a solid, an electric field gradient may also be defined.

Considering the permittivity of a material, which may differ from the permittivity of free space , the electric displacement field is:

[edit] Energy in the electric field

Main article: Electrical energy

The electric field stores energy. The energy density of the electric field is given by

where

is the permittivity of the medium in which the field exists

is the electric field vector.

The total energy stored in the electric field in a given volume V is therefore

where

dV is the differential volume element.

[edit] Parallels between electrostatics and gravity

Coulomb's law, which describes the interaction of electric charges:

is similar to Newton's law of universal gravitation:

This suggests similarities between the electric field E and the gravitational field g, so sometimes mass is called "gravitational charge".

Similarities between electrostatic and gravitational forces:

1. Both act in a vacuum.
2. Both are central and conservative.
3. Both obey an inverse-square law (both are inversely proportional to square of r).
4. Both propagate with finite speed c.

Differences between electrostatic and gravitational forces:

1. Electrostatic forces are much greater than gravitational forces (by about 10³⁶ times).
2. Gravitational forces are attractive for like charges, whereas electrostatic forces are repulsive for like charges.
3. There are no negative gravitational charges (no negative mass) while there are both positive and negative electric charges. This difference combined with previous implies that gravitational forces are always attractive, while electrostatic forces may be either attractive or repulsive.
4. Electric charge is invariant while relativistic mass is not.

 

Electric Field

 

전기를 띤 전하나 시간에 따라 변하는 자기장 주위의 공간에는 전기장이 형성된다. 이 전기장 안에서 하전된 물체는 전기력을 받게 된다. 전기장은 패러데이(Michael Faraday)가 처음 소개한 물리량으로 전장 또는 전계라고도 한다. 전기장은 보통 기호 E로 표시하며, 크기와 방향을 갖는 벡터량이다. 국제표준단위계의 단위로 N/C(newton per coulomb), 혹은 V/m(volt per meter)를 사용한다.
 
정전기에서는 단위 전하에 작용하는 전기적인 힘을 전기장으로 정의한다. 전기장의 방향은 양전하에서 나가서 음전하로 들어오는 방향이며 이것이 곧 힘의 방향이기도 하다. 전기장의 크기는 전하의 크기에 대한 전기력으로 정의한다. 곧 전기장은 힘과 전하량 사이의 비례상수가 된다. 식으로 표현하면 E=F/q(굵은 글자는 벡터를 의미한다.)이며, 이것이 쿨롱의 법칙이다. (쿨롱의 법칙은 정전기에서의 전기장만 설명할 수 있을 뿐, 전하의 움직임이 있을 경우는 로렌츠의 법칙으로 전기장을 설명할 수 있다.) 여러 개의 전하가 분포되어 있을 경우에, 전기장은 전하들의 상대적인 위치와 크기에 따라서 결정되며, 각각의 전하에 의한 전기장의 벡터합과 같다. 또한 전기장 내의 한 위치에서의 전기장의 크기는 전하로부터 거리의 제곱에 반비례한다.

한편 움직이는 전하는 전기장과 함께 자기장도 만들어내는데, 자기장이 시간에 따라 변할 경우 전기장을 만들어낸다. 이것을 이차전기장(secondary electric field)이라고 하며 패러데이의 유도법칙을 사용하여 계산할 수 있다. 일반적으로 전기장과 자기장은 완전히 분리되지 않기 때문에 전자기장이라고 한다.
 
전기장 내에 탐색전하(test charge)가 있을 경우, 탐색전하는 공간의 각 점에서 전기장 방향으로 이동한다. 이 방향을 이어가면 하나의 곡선을 얻을 수 있으며, 곡선상 각 점에서의 접선은 그 점에서의 전기장의 방향을 나타낸다. 전기장의 방향을 그린 전기력선과 전위가 같은 점을 이은 등전위면을 통해 전기장의 분포상황을 나타낼 수 있다.
 
전기장 내에는 그 전기장을 발생시키기 위해 공급된 에너지가 존재하며 전기장의 제곱에 비례한다. 즉, 단위부피당의 정전기에너지 u는 공간의 유전율이 ε일 때, u=(1/2)εE²으로 주어진다. 양자역학에서는 전자기장에서의 매개입자를 광자(photon)라고 하며, 광자의 에너지는 hv(h는 플랑크 상수, v는 진동수이다.)로 양자화되어 있다.