Lorentz force: Difference between revisions
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where ''k'' is a constant depending on the units. In [[SI]] units ''k'' = 1; in Gaussian units ''k'' = 1/''c'', where ''c'' is the speed of light in vacuum (299 792 458 m s<sup>−1</sup> exactly). | where ''k'' is a constant depending on the units. In [[SI]] units ''k'' = 1; in Gaussian units ''k'' = 1/''c'', where ''c'' is the speed of light in vacuum (299 792 458 m s<sup>−1</sup> exactly). | ||
The quantity ''q'' is the electric charge of the particle and '''v''' is its velocity. The vector '''B''' is the [[magnetic induction]] (sometimes referred to as the magnetic field). The product of '''v''' and '''B''' is the [[vector product]] (a vector with the direction given by the right hand rule mentioned above and of magnitude ''v B'' sin α with α the angle between '''v''' | The quantity ''q'' is the electric charge of the particle and '''v''' is its velocity. The vector '''B''' is the [[magnetic induction]] (sometimes referred to as the magnetic field). The product of '''v''' and '''B''' is the [[vector product]] (a vector with the direction given by the right hand rule mentioned above and of magnitude ''v B'' sin α with α the angle between '''v''' and '''B'''). | ||
The electric field '''E''' is given by | The electric field '''E''' is given by | ||
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where ''k'' = 1 for SI units and 1/''c'' for Gaussian units. In this form the Lorentz force was given by [[Oliver Heaviside]] in 1889, three years before Lorentz.<ref>E. Whittaker, ''A History of the Theories of Aether and Electricity'', vol. I, 2nd edition, Nelson, London (1951). Reprinted by the American Institute of Physics, (1987). p. 310 </ref> | where ''k'' = 1 for SI units and 1/''c'' for Gaussian units. In this form the Lorentz force was given by [[Oliver Heaviside]] in 1889, three years before Lorentz.<ref>E. Whittaker, ''A History of the Theories of Aether and Electricity'', vol. I, 2nd edition, Nelson, London (1951). Reprinted by the American Institute of Physics, (1987). p. 310 </ref> | ||
In [[special relativity]] the Lorentz force transforms as a vector under a [[Lorentz transformation]], giving a linear combination of '''E''' and '''B'''. | In [[special relativity]] the Lorentz force transforms as a vector under a [[Lorentz transformation]], giving a linear combination of '''E''' and '''B''', because relativistically the fields '''E''' and '''B''' are components of the same second rank tensor and do not have an independent existence.<ref>J. D. Jackson, ''Classical Electrodynamics'', John Wiley, New York, 2nd ed. (1975), p. 553</ref> | ||
==Notes== | ==Notes== | ||
<references /> | <references /> | ||
Revision as of 01:57, 13 May 2008
In physics the Lorentz force is the force on an electrically charged particle that moves through a magnetic field B and an electric field E.
The strength of the magnetic component of the Lorentz force is proportional to the charge q of the particle, the speed v (the size of the velocity v) of the particle, the intensity B of the magnetic field, and the sine of the angle between the vectors v and B. The direction of the magnetic component is given by the right hand rule: put your right hand along v with fingers pointing in the direction of v and the open palm toward the magnetic field B (a vector). Stretch the thumb of your right hand, then the Lorentz force is along it, pointing from your wrist to the tip of your thumb.
The electric component of the Lorentz force is equal to q E, which must be added vectorially to the magnetic component in order to obtain the total Lorentz force.
The force is named after the Dutch physicist Hendrik Antoon Lorentz, who gave its description in 1892.[1]
Mathematical description
The Lorentz force F is given by the expression
where k is a constant depending on the units. In SI units k = 1; in Gaussian units k = 1/c, where c is the speed of light in vacuum (299 792 458 m s−1 exactly). The quantity q is the electric charge of the particle and v is its velocity. The vector B is the magnetic induction (sometimes referred to as the magnetic field). The product of v and B is the vector product (a vector with the direction given by the right hand rule mentioned above and of magnitude v B sin α with α the angle between v and B). The electric field E is given by
where V is a scalar (electric) potential and the (magnetic) vector potential A is connected to B via
The factor k has the same meaning as before. The operator ∇ acting on V gives the gradient of V, while ∇ × A is the curl of A.
If B is static (does not depend on time) then A is also static and
Non-relativistically, the electric field E may be absent (zero) while B is static and non-zero; the Lorentz force is then given by,
where k = 1 for SI units and 1/c for Gaussian units. In this form the Lorentz force was given by Oliver Heaviside in 1889, three years before Lorentz.[2]
In special relativity the Lorentz force transforms as a vector under a Lorentz transformation, giving a linear combination of E and B, because relativistically the fields E and B are components of the same second rank tensor and do not have an independent existence.[3]
Notes
- ↑ H. A. Lorentz, La théorie électromagnétique de Maxwell et son application aux corps mouvants [The electromagnetic theory of Maxwell and its application to moving bodies], Archives néerlandaises des Sciences exactes et naturelles, vol. 25 p. 363 (1892).
- ↑ E. Whittaker, A History of the Theories of Aether and Electricity, vol. I, 2nd edition, Nelson, London (1951). Reprinted by the American Institute of Physics, (1987). p. 310
- ↑ J. D. Jackson, Classical Electrodynamics, John Wiley, New York, 2nd ed. (1975), p. 553