potential reserves - definitie. Wat is potential reserves
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Wat (wie) is potential reserves - definitie

RELATIVISTIC VECTOR FIELD
Electromagnetic potential; 4-potential; Four-potential; 4-potential A; Four vector potential; Electromagnetic four potential

Electric potential         
  • The electric potential created by a charge, ''Q'', is ''V''&nbsp;=&thinsp;''Q''/(4πε<sub>0</sub>''r''). Different values of ''Q'' yield different values of electric potential, ''V'', (shown in the image).
LINE INTEGRAL OF THE ELECTRIC FIELD
Electrical potential; Electrostatic potential; Electric scalar potential; Electrical scalar potential; Electrical potential difference; Electric Scalar Potential; Coulomb potential; Coulomb Potential; Electric Potential; Electrical Potential; Potential electric; Scalar potential difference; Vector potential difference; Electric field potential
The electric potential (also called the electric field potential, potential drop, the electrostatic potential) is defined as the amount of work energy needed to move a unit of electric charge from a reference point to the specific point in an electric field. More precisely, it is the energy per unit charge for a test charge that is so small that the disturbance of the field under consideration is negligible.
Scalar potential         
  • Vector field (right) and corresponding scalar potential (left).
  • Plot of a two-dimensional slice of the gravitational potential in and around a uniform spherical body. The [[inflection point]]s of the cross-section are at the surface of the body.
  • uniform gravitational field near the Earth's surface
CONCEPT IN VECTOR ANALYSIS AND PHYSICS
Scalar Potential; Scaler potential
In mathematical physics, scalar potential, simply stated, describes the situation where the difference in the potential energies of an object in two different positions depends only on the positions, not upon the path taken by the object in traveling from one position to the other. It is a scalar field in three-space: a directionless value (scalar) that depends only on its location.
Electromagnetic four-potential         
An electromagnetic four-potential is a relativistic vector function from which the electromagnetic field can be derived. It combines both an electric scalar potential and a magnetic vector potential into a single four-vector.

Wikipedia

Electromagnetic four-potential

An electromagnetic four-potential is a relativistic vector function from which the electromagnetic field can be derived. It combines both an electric scalar potential and a magnetic vector potential into a single four-vector.

As measured in a given frame of reference, and for a given gauge, the first component of the electromagnetic four-potential is conventionally taken to be the electric scalar potential, and the other three components make up the magnetic vector potential. While both the scalar and vector potential depend upon the frame, the electromagnetic four-potential is Lorentz covariant.

Like other potentials, many different electromagnetic four-potentials correspond to the same electromagnetic field, depending upon the choice of gauge.

This article uses tensor index notation and the Minkowski metric sign convention (+ − − −). See also covariance and contravariance of vectors and raising and lowering indices for more details on notation. Formulae are given in SI units and Gaussian-cgs units.

Voorbeelden uit tekstcorpus voor potential reserves
1. The potential reserves in some cases are gigantic.
2. The acreage on offer contains potential reserves of an estimated 6.2 billion barrels, including light and heavy oil.
3. In August 2004, then–oil minister Thamer Ghadhban said Iraq had "unconfirmed or potential" reserves of 214bn barrels.
4. The cost of that exploration is estimated at $140 million and has predicted potential reserves of 87 billion cubic meters (bcm) – triple those of the Yam Thetis project.
5. Lorentz said Pearl‘s proven reserves stand at 14 million barrels, potential reserves at 28 million barrels and undeveloped gas reserves at 386 billion cubic feet.