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In the theory of relativity, a four-vector is a vector in a four-dimensional real vector space, called Minkowski space. It differs from a vector in that it can be transformed by Lorentz transformations. The usage of the four-vector name tacitly assumes that its components refer to a standard basis. The components transform between these bases as the space and time coordinate differences, (cΔtxy z) under spatial translations, rotations, and boosts (a change by a constant velocity to another inertial reference frame). The set of all such translations, rotations, and boosts (called Poincaré transformations) forms the Poincaré group. The set of rotations and boosts (Lorentz transformations, described by 4×4 matrices) forms the Lorentz group.

This article considers four-vectors in the context of special relativity. Although the concept of four-vectors also extends to general relativity, some of the results stated in this article require modification in general relativity.

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Mathematics of four-vectors

A point in Minkowski space is called an "event" and is described in a standard basis by a set of four coordinates such as

 \mathbf{X} := \left(X^0, X^1, X^2, X^3 \right) = \left(ct, x, y, z \right)

where μ = 0, 1, 2, 3, labels the spacetime dimensions and where c is the speed of light. The definition X0 = ct ensures that all the coordinates have the same units (of distance).[1][2][3] These coordinates are the components of the position four-vector for the event. The displacement four-vector is defined to be an "arrow" linking two events:

 \Delta \mathbf{X}:= \left(\Delta ct, \Delta x, \Delta y, \Delta z \right)

(Note that the position vector is the displacement vector when one of the two events is the origin of the coordinate system. Position vectors are relatively trivial; the general theory of four-vectors is concerned with displacement vectors.)

The scalar product of two four-vectors \mathbf{U} and \mathbf{V} is defined (using Einstein notation) as

 \mathbf{U \cdot V} = \eta_{\mu \nu} U^{\mu} V^{\nu} = \left( \begin{matrix}U^0 & U^1 & U^2 & U^3 \end{matrix} \right) \left( \begin{matrix} 1 & 0 & 0 & 0 \\ 0 & -1 & 0 & 0 \\ 0 & 0 & -1 & 0 \\ 0 & 0 & 0 & -1 \end{matrix} \right) \left( \begin{matrix}V^0 \\ V^1 \\ V^2 \\ V^3 \end{matrix} \right) = U^0 V^0 - U^1 V^1 - U^2 V^2 - U^3 V^3

where η is the Minkowski metric. Sometimes this inner product is called the Minkowski inner product. It is not a true inner product in the mathematical sense because it is not positive definite. Note: some authors define η with the opposite sign:

 \eta_{\mu \nu} = \left( \begin{matrix} -1 & 0 & 0 & 0 \\ 0 & 1 & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \end{matrix} \right)

in which case

 \mathbf{U \cdot V} = -U^0 V^0 + U^1 V^1 + U^2 V^2 + U^3 V^3

An important property of the inner product is that it is invariant (that is, a scalar): a change of coordinates does not result in a change in value of the inner product.

The inner product is often expressed as the effect of the dual vector of one vector on the other:

\mathbf{U \cdot V} = U^*(\mathbf{V}) = U{_\nu}V^{\nu}

Here the Uνs are the components of the dual vector U * of \mathbf{U} in the dual basis and called the covariant coordinates of \mathbf{U}, while the original Uν components are called the contravariant coordinates. Lower and upper indices indicate always covariant and contravariant coordinates, respectively.

The relation between the covariant and contravariant coordinates is:

U_{\mu} = \eta_{\mu \nu} U^{\nu} \,.

The four-vectors are arrows on the spacetime diagram or Minkowski diagram. In this article, four-vectors will be referred to simply as vectors.

Four-vectors may be classified as either spacelike, timelike or null. Spacelike, timelike, and null vectors are ones whose inner product with themselves is less than, greater than, and equal to zero respectively (assuming Minkowski metric with signature (+,-,-,-)).

In special relativity (but not general relativity), the derivative of a four-vector with respect to a scalar (invariant) is itself a four-vector.

Examples of four-vectors in dynamics

When considering physical phenomena, differential equations arise naturally; however, when considering space and time derivatives of functions, it is unclear which reference frame these derivatives are taken with respect to. It is agreed that time derivatives are taken with respect to the proper time (τ). As proper time is an invariant, this guarantees that the proper-time-derivative of any four-vector is itself a four-vector. It is then important to find a relation between this proper-time-derivative and another time derivative (using the time of an inertial reference frame). This relation is provided by the time transformation in the Lorentz transformations and is:

\frac{d \tau}{dt}=\frac{1}{\gamma}

where γ is the Lorentz factor. Important four-vectors in relativity theory can now be defined, such as the four-velocity of an \mathbf{X}(\tau) world line is defined by:

\mathbf{U} := \frac{d\mathbf{X}}{d \tau}= \frac{d\mathbf{X}}{dt}\frac{dt}{d \tau}= \left(\gamma c, \gamma \mathbf{u} \right),

where, using suffix notation,

\mathbf{u} = u^i = \frac{dX^i}{dt}

for i = 1, 2, 3. Notice that

 || \mathbf{U} ||^2 = U^{\mu} U_{\mu} = c^2 \,

The four-acceleration is given by:

\mathbf{A} =\frac{d\mathbf{U} }{d \tau} = \left(\gamma \dot{\gamma} c, \gamma \dot{\gamma} \mathbf{u} + \gamma^2 \dot{\mathbf{u}} \right)

Since the magnitude  \sqrt{ | U_\mu U^\mu | } of  \mathbf{U} is a constant, the four acceleration is (pseudo-)orthogonal to the four velocity, i.e. the Minkowski inner product of the four-acceleration and the four-velocity is zero:

 A_\mu U^\mu =\frac{1}{2} \frac{\partial (U^\mu U_\mu)}{\partial \tau } = 0 \,

which is true for all world lines .

The four-momentum for a massive particle is given by:

\mathbf{P} :=m \mathbf{U} = (\gamma mc, \mathbf{p}) = (\gamma mc, \gamma m\mathbf{u})

where m is the invariant mass of the particle and p is the relativistic momentum.

The four-force is defined by:

 \mathbf{F} := \frac {d \mathbf{P}} {d \tau}

For a particle of constant mass, this is equivalent to

 \mathbf{F} = m \mathbf{A} = \left(\gamma \dot{\gamma} mc, \gamma \mathbf{f} \right)

where

 \mathbf{f} = \frac{d\mathbf{p}}{dt} = \dot{\gamma} m\mathbf{u} + \gamma m\dot{\mathbf{u}} .

Physics of four-vectors

The power and elegance of the four-vector formalism may be demonstrated by seeing that known relations between energy and matter are embedded into it.

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E = mc2

Here, an expression for the total energy of a particle will be derived. The kinetic energy (K) of a particle is defined analogously to the classical definition, namely as

 \frac{dK}{dt}= \mathbf{f} \cdot \mathbf{u}

with f as above. Noticing that FμUμ = 0 and expanding this out we get

 \gamma^2 \left(\mathbf{f} \cdot \mathbf{u} - \dot{\gamma} mc^2 \right) = 0

Hence

 \frac{dK}{dt} = c^2 \frac{d\gamma m}{dt}

which yields

 K = \gamma m c^2 + S \,

for some constant S. When the particle is at rest (u = 0), we take its kinetic energy to be zero (K = 0). This gives

 S = -m c^2 \,

Thus, we interpret the total energy E of the particle as composed of its kinetic energy K and its rest energy m c2. Thus, we have

 E = \gamma m c^2 \,

E2 = p2c2 + m2c4

Using the relation E = γmc2, we can write the four-momentum as

 \mathbf{P} = \left(\frac{E}{c}, \mathbf{p} \right).

Taking the inner product of the four-momentum with itself in two different ways, we obtain the relation

 \frac{E^2}{c^2} - p^2 = P^\mu P_\mu = m^2 U^\mu U_\mu = m^2 c^2

i.e.

 \frac{E^2}{c^2} - p^2 = m^2 c^2

Hence

 E^2 = p^2 c^2 + m^2 c^4 \,

This last relation is useful in many areas of physics.

Examples of four-vectors in electromagnetism

Examples of four-vectors in electromagnetism include the four-current defined by

 \mathbf{J} := \left( \rho c, \mathbf{j} \right)

formed from the current density j and charge density ρ, and the electromagnetic four-potential defined by

 \mathbf{\Psi} := \left( \phi , \mathbf{a} c \right)

formed from the vector potential a and the scalar potential \phi \,.

A plane electromagnetic wave can be described by the four-frequency defined as

\mathbf{N} :=\left(\nu, \nu \mathbf{n} \right)

where ν is the frequency of the wave and n is a unit vector in the travel direction of the wave. Notice that

 N^\mu N_\mu = \nu ^2 \left(n^2 - 1 \right) = 0

so that the four-frequency is always a null vector.

A wave packet of nearly monochromatic light can be characterized by the wave vector, or four-wavevector

\mathbf{K} = \left(\frac{\omega}{c}, \mathbf{k} \right) \,

See also

References

  1. ^ Jean-Bernard Zuber & Claude Itzykson, Quantum Field Theory, pg 5 , ISBN 0070320713
  2. ^ Charles W. Misner, Kip S. Thorne & John A. Wheeler,Gravitation, pg 51, ISBN 0716703440
  3. ^ George Sterman, An Introduction to Quantum Field Theory, pg 4 , ISBN 0521311322
  • Rindler, W. Introduction to Special Relativity (2nd edn.) (1991) Clarendon Press Oxford ISBN 0-19-853952-5

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