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| '''Earnshaw's theorem''' states that a collection of [[point charge]]s cannot be maintained in a stable stationary [[mechanical equilibrium|equilibrium]] configuration solely by the [[electrostatic]] interaction of the charges. This was first proven by British mathematician [[Samuel Earnshaw]] in 1842. It is usually referenced to [[magnetic field]]s, but was first applied to [[electrostatic field]]s.
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| Earnshaw's theorem applies to classical [[inverse-square law]] [[force]]s (electric and [[gravitational field|gravitational]]) and also to the magnetic forces of [[permanent magnet]]s, if the magnets are hard (the magnets do not vary in strength with external fields). Earnshaw's theory forbids [[magnetic levitation]] in many common situations.
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| If the materials are not hard, [[Werner Braunbeck|Braunbeck]]'s extension shows that materials with relative [[magnetic permeability]] greater than one are further destabilising, but materials with a permeability less than one- [[diamagnetism|diamagnetic]] materials- permit stable configurations.
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| == Explanation ==
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| Informally, the case of a point charge in an arbitrary static electric field is a simple consequence of [[Gauss's law]]. For a particle to be in a stable equilibrium, small perturbations ("pushes") on the particle in any direction should not break the equilibrium; the particle should "fall back" to its previous position. This means that the force field lines around the particle's equilibrium position should all point inwards, towards that position. If all of the surrounding field lines point towards the equilibrium point, then the [[divergence]] of the field at that point must be negative (i.e. that point acts as a sink). However, Gauss's Law says that the divergence of any possible electric force field is zero in free space. In mathematical notation, an electrical force '''F'''('''r''') deriving from a potential ''U''('''r''') will always be divergenceless (satisfy [[Laplace's equation]]):
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| : <math>\nabla \cdot \mathbf{F} = \nabla \cdot (-\nabla U) = -\nabla^2 U = 0.</math> | |
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| Therefore, there are no local [[minimum|minima]] or [[maximum|maxima]] of the field potential in free space, only [[saddle point]]s. A stable equilibrium of the particle cannot exist and there must be an instability in at least one direction.
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| To be completely rigorous, strictly speaking, the existence of a stable point does not require that all neighboring force vectors point exactly toward the stable point; the force vectors could spiral in towards the stable point, for example. One method for dealing with this invokes the fact that, in addition to the divergence, the [[Curl (mathematics)|curl]] of any electric field in free space is also zero (in the absence of any magnetic currents).
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| It is also possible to prove this theorem directly from the force/energy equations for static [[magnetic dipole]]s (below). Intuitively, though, it's plausible that if the theorem holds
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| for a single point charge then it would also hold for two opposite point charges connected together. In particular, it would hold in the limit where the distance between the charges is decreased to zero while maintaining the dipole moment - that is, it would hold for an [[electric dipole]]. But if the theorem holds for an electric dipole then it will also hold for a magnetic dipole since the (static) force/energy equations take the same form for both electric and magnetic dipoles.
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| As a practical consequence, then, this theorem also states that there is no possible static configuration of [[ferromagnet]]s which can stably [[levitate]] an object against gravity, even when the magnetic forces are stronger than the gravitational forces.
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| Earnshaw's theorem has even been proven for the general case of extended bodies, and this is so even if they are flexible and conducting, provided they are not [[diamagnetic]],<ref>{{cite web |url = http://www.ru.nl/hfml/research/levitation/diamagnetic/levitation_possible/ |title = Is Magnetic Levitation Possible? |publisher = High Field Magnet Laboratory |author = Gibbs, Philip & Geim, Andre |accessdate = 2010-01-04}}</ref><ref>Earnshaw, S., On the nature of the molecular forces which regulate the constitution of the luminferous ether., Trans. Camb. Phil. Soc., 7, pp 97-112 (1842)</ref> as diamagnetism constitutes a (small) repulsive force, but no attraction.
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| There are, however, several exceptions to the rule's assumptions which allow [[magnetic levitation]].
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| ==Loopholes==
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| Earnshaw's theorem has no exceptions for non-moving permanent [[Ferromagnetism|ferromagnets]]. However, Earnshaw's theorem does not necessarily apply to moving ferromagnets,<ref name=AJOP/> certain electromagnetic systems, pseudo-levitation and diamagnetic materials. These can thus seem to be exceptions, though in fact they exploit the constraints of the theorem.
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| Spinning ferromagnets (such as the [[Levitron]]) can—while spinning—magnetically levitate using only permanent ferromagnets.<ref name=AJOP>[http://www.physics.ucla.edu/marty/levitron/] American Journal of Physics, April 1997 Spin stabilized magnetic levitation Martin D. Simon, UCLA Department of Physics</ref> Note that since this is spinning, this is not a non-moving ferromagnet.
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| Switching the polarity of an electromagnet or system of electromagnets can levitate a system by continuous expenditure of energy. [[Maglev (transport)|Maglev trains]] are one application.
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| [[Pseudo-levitation]] constrains the movement of the magnets usually using some form of a tether or wall. This works because the theorem shows only that there is some direction in which there will be an instability. Limiting movement in that direction allows for levitation with fewer than the full 3 dimensions available for movement (note that the theorem is proven for 3 dimensions, not 1D or 2D).
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| [[Diamagnetism|Diamagnetic]] materials are excepted because they exhibit only repulsion against the magnetic field, whereas the theorem requires materials that have both repulsion and attraction. A fun example of this is the famous [[Magnetic levitation#Direct_diamagnetic_levitation|levitating frog]] (see [[diamagnetism]]).
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| ==Effect on physics==
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| Configurations of classical charged particles orbiting one another are unstable due to losses of energy by electromagnetic radiation. Even without those losses, Earnshaw’s theorem means that dynamic systems of charges are unstable over long periods. For quite some time, this led to the puzzling question of why matter stays together as much evidence was found that matter was held together electromagnetically, but static configurations would be unstable, and electrodynamic configurations would be expected to radiate energy and decay.
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| These questions eventually pointed the way to [[quantum mechanics|quantum mechanical]] explanations of the structure of the atom, and it turns out that the [[Pauli exclusion principle]] and the existence of discrete electron orbitals is responsible for making bulk matter rigid.
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| ==Proofs for magnetic dipoles==
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| ===Introduction===
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| While a more general proof may be possible, three specific cases are considered here. The first case is a magnetic dipole of constant magnitude that has a fast (fixed) orientation. The second and third cases are magnetic dipoles where the orientation changes to remain aligned either parallel or antiparallel to the field lines of the external magnetic field. In paramagnetic and diamagnetic materials the dipoles are aligned parallel and antiparallel to the field lines, respectively.
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| ===Background===
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| The proofs considered here are based on the following principles.
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| The energy U of a [[magnetic dipole]] with a [[magnetic dipole moment]] '''M''' in an external magnetic field '''B''' is given by
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| :<math>U = -\mathbf{M}\cdot\mathbf{B} = -(M_x B_x + M_y B_y + M_z B_z).</math>
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| The dipole will only be stably levitated at points where the energy has a minimum. The energy can only have a minimum at points where the Laplacian of the energy is greater than zero. That is, where
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| :<math>\nabla^2 U = \frac{\partial^2 U}{\partial x^2} + \frac{\partial^2 U}{\partial y^2} + \frac{\partial^2 U}{\partial z^2} > 0.</math>
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| Finally, because both the divergence and the curl of a magnetic field are zero (in the absence of current or a changing electric field), the Laplacians of the individual components of a magnetic field are zero. That is,
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| :<math>\nabla^2 B_x = \nabla^2 B_y = \nabla^2 B_z = 0.</math>
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| This is proven at the very end of this article as it is central to understanding the overall proof.
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| ===Summary of proofs===
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| For a magnetic dipole of fixed orientation (and constant magnitude) the energy will be given by
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| :<math>U = -\mathbf{M}\cdot\mathbf{B} = -(M_x B_x + M_y B_y + M_z B_z),</math>
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| where ''M<sub>x</sub>'', ''M<sub>y</sub>'' and ''M<sub>z</sub>'' are constant. In this case the Laplacian of the energy is always zero,
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| :<math>\nabla^2 U = 0,</math>
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| so the dipole can have neither an energy minimum or an energy maximum. That is, there is no point in free space where the dipole is either stable in all directions or unstable in all directions.
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| Magnetic dipoles aligned parallel or antiparallel to an external field with the magnitude of the dipole proportional to the external field will correspond to paramagnetic and diamagnetic materials respectively. In these cases the energy will be given by
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| :<math>U = -\mathbf{M}\cdot\mathbf{B} = -k\mathbf{B}\cdot\mathbf{B} = -k \left (B_x^2 + B_y^2 + B_z^2 \right ),</math>
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| where ''k'' is a constant greater than zero for paramagnetic materials and less than zero for diamagnetic materials.
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| In this case, it will be shown that
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| :<math>\nabla^2 \left (B_x^2 + B_y^2 + B_z^2 \right ) \geq 0,</math>
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| which, combined with the constant ''k'', shows that paramagnetic materials can have energy maxima but not energy minima and diamagnetic materials can have energy minima but not energy maxima. That is, paramagnetic materials can be unstable in all directions but not stable in all directions and diamagnetic materials can be stable in all directions but not unstable in all directions. Of course, both materials can have saddle points.
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| Finally, the magnetic dipole of a ferromagnetic material (a permanent magnet) that is aligned parallel or antiparallel to a magnetic field will be given by
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| :<math>\mathbf{M} = k{\mathbf{B} \over |\mathbf{B}|},</math>
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| so the energy will be given by
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| :<math>U = -\mathbf{M}\cdot\mathbf{B} = -k{{\mathbf{B}\cdot\mathbf{B}} \over |\mathbf{B}|} = -k{|\mathbf{B}|^2 \over |\mathbf{B}|} = -k\left (B_x^2 + B_y^2 + B_z^2 \right )^{\frac{1}{2}};</math>
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| but this is just the square root of the energy for the paramagnetic and diamagnetic case discussed above and, since the square root function is monotonically increasing, any minimum or maximum in the paramagnetic and diamagnetic case will be a minimum or maximum here as well. There are, however, no known configurations of permanent magnets that stably levitate so there may be other reasons not discussed here why it is not possible to maintain permanent magnets in orientations antiparallel to magnetic fields (at least not without rotation—see [[Levitron]]).
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| ===Detailed proofs===
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| Earnshaw's theorem was originally formulated for electrostatics (point charges) to show that there is no stable configuration of a collection of point charges. The proofs presented here for individual dipoles should be generalizable to collections of magnetic dipoles because they are formulated in terms of energy, which is additive. A rigorous treatment of this topic is, however, currently beyond the scope of this article.
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| ===Fixed-orientation magnetic dipole===
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| It will be proven that at all points in free space
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| :<math> \nabla \cdot (\nabla U) = \nabla^2 U = {\partial^2 U \over {\partial x}^2} + {\partial^2 U \over {\partial y}^2} + {\partial^2 U \over {\partial z}^2} = 0.</math>
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| The energy ''U'' of the magnetic dipole '''M''' in the external magnetic field '''B''' is given by
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| :<math>U = -\mathbf{M}\cdot\mathbf{B} = -M_x B_x - M_y B_y - M_z B_z.</math>
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| The Laplacian will be
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| :<math>\nabla^2 U = -{\partial^2 (M_x B_x + M_y B_y + M_z B_z) \over {\partial x}^2} - {\partial^2 (M_x B_x + M_y B_y + M_z B_z) \over {\partial y}^2} - {\partial^2 (M_x B_x + M_y B_y + M_z B_z) \over {\partial z}^2}</math>
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| Expanding and rearranging the terms (and noting that the dipole '''M''' is constant) we have
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| :<math>\begin{align}
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| \nabla^2 U &= -M_x\left({\partial^2 B_x \over {\partial x}^2} + {\partial^2 B_x \over {\partial y}^2} + {\partial^2 B_x \over {\partial z}^2}\right) - M_y\left({\partial^2 B_y \over {\partial x}^2} + {\partial^2 B_y \over {\partial y}^2} + {\partial^2 B_y \over {\partial z}^2}\right) - M_z\left({\partial^2 B_z \over {\partial x}^2} +{\partial^2 B_z \over {\partial y}^2} +{\partial^2 B_z \over {\partial z}^2}\right)\\
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| &= -M_x \nabla^2 B_x - M_y \nabla^2 B_y - M_z \nabla^2 B_z
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| \end{align}</math>
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| but the Laplacians of the individual components of a magnetic field are zero in free space (not counting electromagnetic radiation) so
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| :<math>\nabla^2 U = -M_x 0 - M_y 0 - M_z 0 = 0,</math>
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| which completes the proof.
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| ===Magnetic dipole aligned with external field lines===
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| The case of a paramagnetic or diamagnetic dipole is considered first. The energy is given by
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| :<math>U = -k|\mathbf{B}|^2 = -k \left (B_x^2 + B_y^2 + B_z^2 \right ).</math>
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| Expanding and rearranging terms,
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| :<math>\begin{align}
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| \nabla^2 |\mathbf{B}|^2 &= \nabla^2 \left (B_x^2 + B_y^2 + B_z^2 \right ) \\
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| &= 2\left( |\nabla B_x|^2 + |\nabla B_y|^2 + |\nabla B_z|^2 +B_x\nabla^2 B_x + B_y\nabla^2 B_y + B_z\nabla^2 B_z \right)
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| \end{align}</math>
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| but since the Laplacian of each individual component of the magnetic field is zero,
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| :<math>\nabla^2 |\mathbf{B}|^2 = 2\left( | \nabla B_x |^2 + | \nabla B_y |^2 + | \nabla B_z |^2 \right);</math>
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| and since the square of a magnitude is always positive,
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| :<math>\nabla^2 |\mathbf{B}|^2 \geq 0.</math>
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| As discussed above, this means that the Laplacian of the energy of a paramagnetic material can never be positive (no stable levitation) and the Laplacian of the energy of a diamagnetic material can never be negative (no instability in all directions).
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| Further, because the energy for a dipole of fixed magnitude aligned with the external field will be the square root of the energy above, the same analysis applies.
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| ===Laplacian of individual components of a magnetic field===
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| It is proven here that the Laplacian of each individual component of a magnetic field is zero. This shows the need to invoke the properties of magnetic fields that the [[divergence]] of a magnetic field is always zero and the [[curl (mathematics)|curl]] of a magnetic field is zero in free space. (That is, in the absence of current or a changing electric field.) See [[Maxwell's equations]] for a more detailed discussion of these properties of magnetic fields.
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| Consider the Laplacian of the x component of the magnetic field
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| :<math>\begin{align}
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| \nabla^2 B_x &= {\partial^2 B_x \over \partial x^2} + {\partial^2 B_x \over \partial y^2} + {\partial^2 B_x \over \partial z^2}\\
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| &= {\partial \over \partial x} {\partial B_x \over \partial x} + {\partial \over \partial y} {\partial B_x \over \partial y} + {\partial \over \partial z} {\partial B_x \over \partial z}
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| \end{align}</math>
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| Because the curl of '''B''' is zero,
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| :<math>\frac{\partial B_x}{\partial y} = \frac{\partial B_y}{\partial x},</math>
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| and
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| :<math>\frac{\partial B_x}{\partial z} = \frac{\partial B_z}{\partial x},</math>
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| so we have
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| :<math>\nabla^2 B_x = {\partial \over \partial x}{\partial B_x \over \partial x} + {\partial \over \partial y}{\partial B_y \over \partial x} + {\partial \over \partial z}{\partial B_z \over \partial x}.</math>
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| But since ''B<sub>x</sub>'' is continuous, the order of differentiation doesn't matter giving
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| :<math>\nabla^2 B_x = {\partial \over \partial x}\left({\partial B_x \over \partial x} +{\partial B_y \over \partial y} +{\partial B_z \over \partial z} \right) = {\partial \over \partial x}(\nabla \cdot \mathbf{B}).</math>
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| The divergence of '''B''' is zero,
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| :<math>\nabla \cdot \mathbf{B} = 0,</math>
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| so
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| :<math>\nabla^2 B_x = {\partial \over \partial x}(\nabla \cdot \mathbf{B}) = 0.</math>
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| The Laplacian of the ''y'' component of the magnetic field ''B<sub>y</sub>'' field and the Laplacian of the ''z'' component of the magnetic field ''B<sub>z</sub>'' can be calculated analogously. Alternatively, one can use the [[Vector calculus identities|identity]]
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| :<math>\nabla^{2}\mathbf{B} = \nabla(\nabla \cdot \mathbf{B}) - \nabla \times \left( \nabla \times \mathbf{B} \right),</math>
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| where both terms in the parentheses vanish.
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| == Notes ==
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| <references/>
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| == References ==
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| *{{Cite journal |first=Samuel |last=Earnshaw |title=On the Nature of the Molecular Forces which Regulate the Constitution of the Luminiferous Ether |journal=Trans. Camb. Phil. Soc. |volume=7 |issue= |pages=97–112 |year=1842 }}
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| *{{Cite journal |first=W. T. |last=Scott |title=Who Was Earnshaw? |journal=[[American Journal of Physics]] |volume=27 |issue= |pages=418 |year=1959 |bibcode = 1959AmJPh..27..418S |doi = 10.1119/1.1934886 }}
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| == See also ==
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| * [[Magnetic levitation]]
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| * [[Electrostatic levitation]]
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| == External links ==
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| *"[http://www.ru.nl/hfml/research/levitation/diamagnetic/levitation_possible/ Is magnetic levitation possible?]", a discussion of Earnshaw's theorem and its consequences for levitation, along with several ways to levitate with electromagnetic fields
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| *[http://www.chem.yale.edu/~chem125/levitron/Earnshaw.html Biography] and other information about [[Samuel Earnshaw]]
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| [[Category:Electrostatics]]
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| [[Category:Levitation]]
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| [[Category:Physics theorems]]
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