Lorentz force

The fine beam tube demonstrates the effect of the Lorentz force on moving charges (electrons).

Play media file

The ladder swing test shows the Lorentz force on a current-carrying conductor.

The Lorentz force is the force that a charge experiences in a magnetic or electric field. A magnetic field exerts a force on moving charges , while an electric field acts equally on moving and immobile charges. It is named after the Dutch mathematician and physicist Hendrik Antoon Lorentz .

The magnetic component of the force is greatest when the direction of movement of the charge is perpendicular to the magnetic field lines and is zero when the charge is moving along a field line. It always acts perpendicular to the direction of movement of the charge and to the magnetic field lines. Their direction of action can be determined using the three-finger rule . The left hand is used for negative charges and the right hand for positive charges.

The special theory of relativity provides an explanation of the Lorentz force, which is ultimately attributed to electrostatic attraction .

history

The form of the induction law in On physical lines of force (1861) or A dynamic theory of the electromagnetic field (1864) by James Clerk Maxwell contains, from today's perspective, a component that can be regarded as the forerunner of the Lorentz force. The actual treatment of the forces on moving point charges in magnetic fields did not take place until 1881 by JJ Thomson . It still had an incorrect prefactor , the correct form of the Lorentz force was derived from Oliver Heaviside (1889) and Lorentz (1895). ${\displaystyle {\frac {1}{2}}}$

general definition

a) Lorentz force when negative or positive charge carriers move
b) Disturbance of the magnetic field by the moving charge carriers. The particles move into the plane of the drawing, the field and the force lie in the plane of the drawing.

If an electric charge moves with speed through an electromagnetic field, the total Lorentz force acting on the charge is in the broader sense: ${\displaystyle q}$ ${\displaystyle {\vec {v}}}$

${\displaystyle {\vec {F}}={\vec {F_{\text{E}}}}+{\vec {F_{\text{B}}}}=q{\vec {E}}+q{\vec {v}}\times {\vec {B}}}$

${\displaystyle {\vec {F_{\text{E}}}}}$and are the electrical and magnetic components of the Lorentz force in the broader sense, the electrical field strength , the magnetic flux density and the symbol that of the vector or cross product of the vectors involved. ${\displaystyle {\vec {F_{\text{B}}}}}$ ${\displaystyle {\vec {E}}}$ ${\displaystyle {\vec {B}}}$ ${\displaystyle \times }$

The resulting vector of a cross product is always perpendicular to both output vectors , and the scalar product of orthogonal vectors is equal to 0.This results in the case of a non-existent external electric field ( ): ${\displaystyle E=0}$

• When a particle of the charge is deflected in the spatially and temporally constant magnetic field, in contrast to the deflection in the electric field, no work is done, the kinetic energy and thus the orbital speed remain unchanged, because ${\displaystyle q}$

${\displaystyle {\frac {\mathrm {d} W_{\text{kin}}}{\mathrm {d} t}}={\frac {m}{2}}\,{\frac {\mathrm {d} ({\vec {v}}^{2})}{\mathrm {d} t}}=m{\vec {v}}\cdot {\frac {\mathrm {d} {\vec {v}}}{\mathrm {d} t}}={\vec {v}}\cdot m\cdot {\vec {a}}={\vec {v}}\cdot {\vec {F}}=q\,{\vec {v}}\cdot {\bigl (}{\vec {v}}\times {\vec {B}}{\bigr )}=0}$.

This also applies to relativistic particles. In fact, however, the particles emit due to their distraction bremsstrahlung and thereby give energy.

• If the vectors and run parallel or antiparallel to each other, it equals 0. If a charge moves in the direction of the field lines of a magnetic field or exactly in the opposite direction, there is no deflection. ${\displaystyle {\vec {v}}}$ ${\displaystyle {\vec {B}}}$ ${\displaystyle {\vec {F}}}$ ${\displaystyle q}$

On the other hand, if one considers, as is usual in older physics textbooks, only the magnetic component of the above total force as the Lorentz force in the narrower sense , then the following formula applies to its calculation: ${\displaystyle {\vec {F}}}$

${\displaystyle {\vec {F}}_{\text{L}}=q{\vec {v}}\times {\vec {B}}}$

The electrical component of the Lorentz force in the broader sense , which is also considered separately in such a case , is then called the Coulomb force and is calculated as follows:

${\displaystyle {\vec {F}}_{\text{C}}=q{\vec {E}}}$

The symbols and or and denote what corresponds to each other, whereby one or the other convention should be retained if possible for the sake of clarity of the spelling . ${\displaystyle {\vec {F_{\text{B}}}}}$ ${\displaystyle {\vec {F_{\text{L}}}}}$ ${\displaystyle {\vec {F_{\text{E}}}}}$ ${\displaystyle {\vec {F_{\text{C}}}}}$

Formulation of the Lorentz force in the cgs system

In contrast to the above notation of the formula for the Lorentz force , which is based on the international system of measurements customary in electrical engineering and the experimental natural sciences , in theoretical physics, and more generally especially in England and the USA, one writes for the same force in the equivalent, but easily different cgs units ${\displaystyle {\vec {F_{\text{L}}}}}$

${\displaystyle {\vec {F}}_{L}=q_{\text{cgs}}\left({\frac {\vec {v}}{c}}\times {\vec {B}}_{\text{cgs}}\right),}$

or for the Lorentz force in a broader sense

${\displaystyle {\vec {F}}=q_{\text{cgs}}\left({\vec {E}}_{\text{cgs}}+{\frac {\vec {v}}{c}}\times {\vec {B}}_{\text{cgs}}\right),}$

where the quantities and as well as the corresponding SI quantities are largely equivalent, so for the sake of simplicity they are usually also referred to as and as well as without special indices . However, the transformation formulas apply : ${\displaystyle q_{\text{cgs}}}$ ${\displaystyle {\vec {B}}_{\text{cgs}}}$ ${\displaystyle {\vec {E}}_{\text{cgs}}}$ ${\displaystyle q}$ ${\displaystyle {\vec {B}}}$ ${\displaystyle {\vec {E}}}$

${\displaystyle q_{\mathrm {cgs} }=q_{\mathrm {SI} }/{\sqrt {4\pi \varepsilon _{0}}}}$

${\displaystyle {\vec {E}}_{\text{cgs}}={\sqrt {4\pi \varepsilon _{0}}}\cdot {\vec {E}}_{\mathrm {SI} }}$

${\displaystyle {\vec {B}}_{\mathrm {cgs} }={\vec {B}}_{\mathrm {SI} }\cdot c\cdot {\sqrt {4\pi \varepsilon _{0}}}={\vec {B}}_{\mathrm {SI} }\cdot {\sqrt {\frac {4\pi }{\mu _{0}}}}}$

with the dimensional dielectric constant in a vacuum (for the systematic conversion of quantities in SI units into the cgs system and vice versa, see the corresponding section in the article on Maxwell's equations ). ${\displaystyle \varepsilon _{0}}$

Ambiguous designation

The term "Lorentz force" is not used uniformly. Older textbooks usually differentiate between the Lorentz force in the narrower sense and the Coulomb force . The former is exerted by magnetic fields on moving charges, the latter by electric fields on moving or immobile charges. The more recent literature usually understands both forces as a magnetic component and an electrical component of the total force , the Lorentz force in the broader sense . ${\displaystyle {\vec {F_{\text{L}}}}}$ ${\displaystyle {\vec {F_{\text{C}}}}}$ ${\displaystyle {\vec {F_{\text{B}}}}}$ ${\displaystyle {\vec {F_{\text{E}}}}}$ ${\displaystyle {\vec {F_{\text{B}}}}+{\vec {F_{\text{E}}}}}$

Lorentz force on moving point charges

Movement of a point charge  q in a magnetic field perpendicular to its orbit (in this case out of the plane of the drawing): Negative charges (q <0) are shown upwards, positive (q> 0) downwards and neutral (q = 0) ) not distracted at all.

As moving point charges are small free charges such as electrons , protons or other charged elementary particles such. B. alpha particles , but also considered ions that are free in space, z. B. in a vacuum or in a saline solution .

Since the direction of the Lorentz force depends on the sign of the charge , oppositely charged point charges in the same direction of movement are deflected in opposite directions. On the other hand, if the oppositely charged point charges also move in opposite directions (e.g. in a salt solution to which an electrical voltage has been applied), the direction of their magnetic deflection is again the same (see adjacent figures). ${\displaystyle q}$

The amount of the Lorentz force results from

${\displaystyle |{\vec {v}}\times {\vec {B}}|=|{\vec {v}}|\,|{\vec {B}}|\,\sin \alpha }$

to

${\displaystyle |{\vec {F}}_{\text{L}}|=|q|\,|{\vec {v}}|\,|{\vec {B}}|\,\sin \alpha }$

with as the angle between the direction of movement of q and the direction of the magnetic field or its flux density . ${\displaystyle \alpha }$ ${\displaystyle {\vec {B}}}$

If the point charge moves exactly perpendicular to the magnetic field, the following applies : ${\displaystyle \sin \alpha =1}$

${\displaystyle |{\vec {F}}_{\text{L}}|=|q|\,|{\vec {v}}|\,|{\vec {B}}|}$

• 

  Magnetic deflection of the ions sets a salt solution in rotation.

• 

  The speed filter to Vienna is based on balance of power between the Lorentz force and Coulomb force.

Lorentz force on the current-carrying conductor

The current balance measures the Lorentz force on the current-carrying conductor.

The Lorentz force is the central link between electricity and mechanics . If current flows through a conductor that is perpendicular or oblique to the field lines of a surrounding magnetic field, then a force can be determined on the conductor. The deflection in the ladder swing test or the measurements in the current balance experiment illustrate this. The force effect is derived from the Lorentz force acting on a moving point charge; this acts on the individual charge carriers in the conductor.

Lorentz force on the ladder

In order to computationally record the processes mentioned, for the sake of simplicity first consider a straight piece of wire of the directed length , which lies in a time-constant, homogeneous external magnetic field of the flux density . A current of strength that is constant over time flows through the wire , so that its conduction electrons move through the wire at a constant speed and the total charge during the running time ${\displaystyle {\vec {\ell }}}$ ${\displaystyle B}$ ${\displaystyle I}$ ${\displaystyle {\vec {v}}}$ ${\displaystyle t}$

${\displaystyle q=I\,t}$

with speed

${\displaystyle {\vec {v}}={\frac {\vec {\ell }}{t}}}$

transport. Because of this, the sum of the Lorentz forces on all conduction electrons involved in the flow of current and thus on the piece of wire as a whole ${\displaystyle q\,{\vec {v}}=I\,{\vec {\ell }}}$

${\displaystyle {\vec {F_{\text{L}}}}=q\,({\vec {v}}\times {\vec {B}})=I\,({\vec {\ell }}\times {\vec {B}}).}$

The associated equation of absolute value then reads

${\displaystyle |{\vec {F}}_{\text{L}}|=|I|\,|{\vec {\ell }}|\,|{\vec {B}}|\,\sin \alpha }$

with as the angle between the longitudinal direction of the wire and the direction of the magnetic flux density . ${\displaystyle \alpha }$ ${\displaystyle {\vec {B}}}$

If the wire runs exactly perpendicular to the magnetic field, and the equation is simplified to ${\displaystyle \sin \alpha =1}$

${\displaystyle |{\vec {F}}_{\text{L}}|=|I|\,|{\vec {\ell }}|\,|{\vec {B}}|.}$

For curved conductors, the force effect must be calculated by integration, in that the magnetic field is only viewed as constant for infinitesimally small pieces of the conductor. This results in the following formula: ${\displaystyle \mathrm {d} {\boldsymbol {\vec {\ell }}}}$

${\displaystyle {\vec {F_{\text{L}}}}=I\int \mathrm {d} {\boldsymbol {\vec {\ell }}}\times {\vec {B}}}$

Force between two current-carrying conductors

See also : Ampère's law of force

Linking the formula for the Lorentz force on conductors through which current flows with the Biot-Savart law for the magnetic field around conductors through which there is current results in a formula for the force that two thin conductors through which current flow exert on each other, which is also known in the literature as Ampère's law of force ( not to be confused with Ampère's law ).

If the two conductors are thin and parallel opposite each other like the opposite sides of a rectangle , then the simple formula for the amount of force of the forces acting on each other (according to the principle of interaction, equally large) results, already known from the Ampère definition : ${\displaystyle F_{12}}$

${\displaystyle F_{12}=\ell \cdot {\frac {\mu _{0}}{2\pi }}{\frac {I_{1}I_{2}}{r}}}$

The length of the conductors (the same for both conductors), their mutual distance and the current strengths in the two conductors. ${\displaystyle \ell }$ ${\displaystyle r}$ ${\displaystyle I_{1},\,I_{2}}$

Electromagnetic induction

Lorentz force and induction

→ Main article : Electromagnetic induction

Furthermore, the Lorentz force explains the conversion of mechanical movement into electrical voltage. The Lorentz force provides an alternative derivation of the electromagnetic induction instead of the change in flux.

For the sake of simplicity, consider again a straight piece of wire of length , which is now pushed at constant speed across a temporally constant, homogeneous external magnetic field of flux density running perpendicular to it, i.e. in such a way that the longitudinal direction of the wire is also perpendicular . ${\displaystyle l}$ ${\displaystyle {\vec {v}}}$ ${\displaystyle B}$ ${\displaystyle {\vec {v}}}$

As explained above, two forces are balanced in this case, on the one hand the Lorentz force , which shifts the conduction electrons of the wire towards one of its two ends, and on the other hand the Coulomb force acting on the conduction electrons due to the induced charge separation between the two conductor ends electrical voltage: ${\displaystyle {\vec {F_{\text{L}}}}}$ ${\displaystyle {\vec {F_{\text{C}}}}}$

${\displaystyle {\vec {F}}_{\text{L}}+{\vec {F}}_{\text{C}}=0\Leftrightarrow {\vec {F}}_{\text{C}}=-{\vec {F}}_{\text{L}}\Leftrightarrow q\,{\vec {E}}=-q\,({\vec {v}}\times {\vec {B}})}$

Shortening the total charge, which is completely insignificant here, and scalar multiplication with the vector of the directed conductor length ultimately yields the equation for the induction voltage sought : ${\displaystyle q}$ ${\displaystyle {\vec {\ell }}}$ ${\displaystyle U_{\text{ind}}}$

${\displaystyle U_{\mathrm {ind} }={\vec {\ell }}\cdot {\vec {E}}=-{\vec {\ell }}\cdot ({\vec {v}}\times {\vec {B}})=({\vec {\ell }}\times {\vec {B}})\cdot {\vec {v}}}$

If the three vectors are perpendicular to each other in pairs, as requested at the beginning, the late product l · (v × B) is simplified , so that the well-known formula

${\displaystyle U_{\text{ind}}=-|{\vec {\ell }}|\,|{\vec {v}}|\,|{\vec {B}}|}$

results (see also the article Ladder Swing ).

Lenz's rule

Circuit demonstrates Lenz's rule.

Lorentzkraft explains Lenz's rule.

→ Main article : Lenz's rule

If both ends of the moving conductor are bridged with an ohmic resistance of the size R, which, on the other hand, is not moved against the magnetic field, a closed conductor loop is created over which the induction voltage can equalize, so that this and the product are the sum according to Kirchhoff's rule of meshes 0 deliver: ${\displaystyle I_{\text{ind}}\cdot R}$

${\displaystyle U_{\mathrm {ind} }+I_{\text{ind}}\cdot R=0\Leftrightarrow }$

${\displaystyle {I_{\text{ind}}}={\frac {-U_{\text{ind}}}{R}}={\frac {{\vec {\ell }}\cdot ({\vec {v}}\times {\vec {B}})}{R}}={\frac {-({\vec {\ell }}\times {\vec {B}})\cdot {\vec {v}}}{R}}}$

The current flowing through the closed circuit now generates a Lorentz force again, which counteracts the direction of movement. The Lorentz force not only explains the charge separation with which the induction voltage arises, but also the counterforce that is part of Lenz's rule.

In the same way, generators generate voltage and allow currents to flow, thereby converting mechanical power into electrical power. In an electric motor , voltage and current are directed in such a way that it absorbs electrical power and releases it as work that has been done.

Working principle

The Lorentz force results in the Lagrangian formulation of the motion of a charged particle of the charge and the mass from the Lagrangian function ${\displaystyle q}$ ${\displaystyle m}$

${\displaystyle {\mathcal {L}}({\vec {x}},{\vec {v}},t)=-mc^{2}{\sqrt {1-{\frac {{\vec {v}}^{2}}{c^{2}}}}}+q\,{\vec {v}}\cdot {\vec {A}}-q\,\Phi }$.

Here, and are the scalar potential and the vector potential that lead to the electric field strength ${\displaystyle \Phi ({\vec {x}},t)}$ ${\displaystyle {\vec {A}}({\vec {x}},t)}$

${\displaystyle {\vec {E}}=-\nabla \Phi -{\frac {\partial {\vec {A}}}{\partial t}}}$

and the magnetic flux density

${\displaystyle {\vec {B}}=\nabla \times {\vec {A}}}$

belong.

The principle of the stationary action leads to the Euler-Lagrange equations

${\displaystyle {\frac {\mathrm {d} }{\mathrm {d} t}}\nabla _{\vec {v}}{\mathcal {L}}-\nabla _{\vec {x}}{\mathcal {L}}=0}$.

The evaluation of the partial derivatives occurring in the Nabla operators yields:

${\displaystyle {\frac {\mathrm {d} }{\mathrm {d} t}}\left({\frac {m\,{\vec {v}}}{\sqrt {1-{\frac {{\vec {v}}^{2}}{c^{2}}}}}}+q\,{\vec {A}}\right)-q\,\nabla \left({\vec {v}}\cdot {\vec {A}}\right)+q\,\nabla \Phi =0}$

The first term in the round brackets is the (kinetic) momentum (while the entire expression in the first round brackets describes the generalized momentum ) of a particle moving with speed : ${\displaystyle {\vec {v}}}$

${\displaystyle {\vec {p}}={\frac {m\,{\vec {v}}}{\sqrt {1-{\frac {{\vec {v}}^{2}}{c^{2}}}}}}}$

The total time derivative of the vector potential, which is explicitly dependent on the time and on all spatial coordinates, is using the vector relation : ${\displaystyle {\vec {v}}\times (\nabla \times {\vec {A}})=\nabla ({\vec {v}}\cdot {\vec {A}})-({\vec {v}}\cdot \nabla ){\vec {A}}}$

${\displaystyle {\frac {\mathrm {d} }{\mathrm {d} t}}{\vec {A}}=\sum _{i}{\frac {\partial {\vec {A}}}{\partial x_{i}}}{\frac {\mathrm {d} x_{i}}{\mathrm {d} t}}+{\frac {\partial {\vec {A}}}{\partial t}}=({\vec {v}}\cdot \nabla )\mathbf {A} +{\frac {\partial {\vec {A}}}{\partial t}}=-{\vec {v}}\times (\nabla \times {\vec {A}})+\nabla ({\vec {v}}\cdot {\vec {A}})+{\frac {\partial {\vec {A}}}{\partial t}}}$

Inserted results in:

${\displaystyle {\frac {\mathrm {d} {\vec {p}}}{\mathrm {d} t}}-\underbrace {q\,{\vec {v}}\times \left(\nabla \times {\vec {A}}\right)} _{q\,{\vec {v}}\times {\vec {B}}}+\underbrace {q\,\nabla \Phi +q\,{\frac {\partial {\vec {A}}}{\partial t}}} _{-q\,{\vec {E}}}=0}$

This gives the equation of motion as a function of E and B:

${\displaystyle {\frac {\mathrm {d} {\vec {p}}}{\mathrm {d} t}}={\vec {F}}=q\,({\vec {E}}+{\vec {v}}\times {\vec {B}})}$

Examples

Historical definition of the unit of measurement amperes

Effect of force on two directly adjacent conductors

From 1948 to 2019, the Lorentz force was the basis of the internationally valid definition of the SI base unit amperes :

One ampere is a small, "the strength of an unlimited fixed time electric current meters by two parallel in the distance of 1 in a vacuum arranged straight, infinitely long conductor having negligible circular cross-section flowing, electrodynamically the power of  N per m length of conductor between these conductors cause would." ${\displaystyle 2\cdot 10^{-7}}$

The amount of the force results from Ampère's law of force for two straight, neighboring and thin line cables. For two conductors through which the current flows or with a mutual distance , the length-related magnetic Lorentz force is : ${\displaystyle I_{1}}$ ${\displaystyle I_{2}}$ ${\displaystyle r}$ ${\displaystyle F'_{12}}$

${\displaystyle F'_{12}={\frac {\mu _{0}}{2\pi }}{\frac {I_{1}I_{2}}{r}}}$

With a conductor spacing and a current of , the force of per meter of conductor length results from the above definition. The resulting force is attractive here; with opposing currents it would be repulsive. ${\displaystyle r=1\,\mathrm {m} }$ ${\displaystyle I_{1}=I_{2}=1\,\mathrm {A} }$ ${\displaystyle 2\cdot 10^{-7}\,\mathrm {N} }$

Technical applications of the Lorentz force

• Rotating electrical machines such as the electric motor and the electric generator
• Deflection magnets and deflection systems for focusing and deflecting charged particle radiation (for example in the cathode ray tube , in picture tubes , in all circular accelerators )
• Wien filter , which only allows ions of a certain speed to pass
• In magnetic field-dependent resistances, such as in the field plate , with the Hall effect and the Hall sensors based on it
• Magnetohydrodynamic generators and magnetohydrodynamic propulsion
• electrodynamic converters, for example loudspeakers , dynamic microphones , moving coil measuring mechanisms
• magnetic confinement of the plasma in nuclear fusion reactors such as the tokamak and the stellarator
• Contactless flow measurement with Lorentz force anemometry
• Mass spectrometry for chemical and physical analysis

Lorentz forces in nature

• The deflection of the solar wind by the earth's magnetic field in the Van Allen Belt is done by the Lorentz force.

Individual evidence

1. ↑ Thomson, On the electric and magnetic effect produced by the motion of electrified bodies, Philosophical Magazine, Volume 11, 1881, pp. 229-249
2. ^ Heaviside, On the Electromagnetic Effects due to the Motion of Electrification through a Dielectric, Philosophical Magazine, 1889, 324
3. ↑ Lorentz, attempt at a theory of electrical and optical phenomena in moving bodies, 1895
4. ↑ Darrigol, Electrodynamics from Ampère to Einstein, Oxford UP, 2000, pp. 429ff
5. ↑ Classical electrodynamics. Lecture at Heidelberg University, accessed on December 18, 2016.
6. ^ Dieter Meschede : Gerthsen Physics . 23rd edition. Springer, Berlin 2006, ISBN 978-3-540-25421-8 .
7. ↑ Vladimir Dyakonov: Introduction to Physics II for students of natural sciences and dentistry, summer semester 2007. ( Memento of the original from December 19, 2013 in the Internet Archive ) Info: The archive link was automatically inserted and not yet checked. Please check the original and archive link according to the instructions and then remove this notice. Reminder section : rotating electrolyte. (PDF; 317 kB). 
8. ↑ The German expression "Ampèresches Kraftgesetz" occurs in the current literature and teaching, see z. B. Dietmar Petrascheck, Franz Schwabl: Electrodynamics. (Springer, 2nd edition, 2014) or Ampere's Law. (Script on the website of the Humboldt University of Berlin), but comparatively seldom, because a Google search for the term yielded e.g. B. only 58 hits. The English counterpart “Ampère's force law”, on the other hand, is much more common, the expression provides over 2000 hits and has its own (English) Wikipedia article. Accessed on May 19, 2016.
9. ^ Paul A. Tipler , Gene Mosca: Physics for Scientists and Engineers . 2nd Edition. Spektrum Akademischer Verlag, 2004, ISBN 3-8274-1164-5 , p. 907 ff .
10. ^ Grüninger, Landesbildungsserver: The Lenz rule. 2011, accessed December 18, 2013 . 

See also

• Induction law
• Reluctance force

Web links

Commons : Lorentzkraft  - album with pictures, videos and audio files

Wiktionary: Lorentz force  - explanations of meanings, word origins, synonyms, translations

• Java applet for experimenting with the Lorentz force
• Another model in which and can be varied ${\displaystyle q,\,v}$ ${\displaystyle B}$
• Experiments and exercises on the Lorentz force ( LEIFI )
• MIT News article on Lorentz force injector