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Facing a paradox: Earnshaw's theorem in one dimension
Does this example contradict Earnshaw's theorem in one dimension?Classify equilibrium points and find bifurcation points of a non-linear dynamic systemEarnshaw's theorem and springsEarnshaw's theorem for extended conducting bodiesPotential due to charge over infinite grounded plane conductor using the method of imagesRelation between electric field and dipole momentEarnshaw's theorm and Effective potentialDielectric liquid sucked up between two cylinders with a voltage differenceElectrostatics: Induced Boundary Dipole LayerWhy do we assume simply connected domains and continuously differentiable fields in electromagnetism theory?Does this example contradict Earnshaw's theorem in one dimension?
$begingroup$
Consider a one-dimensional situation on a straight line (say, $x$-axis). Let a charge of magnitude $q$ be located at $x=x_0$, the potential satisfies the Poisson's equation $$fracd^2Vdx^2=-fracrho(x)epsilon_0=-fracqdelta(x-x_0)epsilon_0.$$ If $q>0$, $V^primeprime(x_0)<0$, and if $q<0$, $V^primeprime(x_0)>0$. Therefore, it appears that the potential $V$ does have a minimum at $x=x_0$, for $q<0$. Does this imply that $x=x_0$ is a point of stable equilibrium? I must be missing something because this appears to violate Earnshaw's theorem (or it doesn't)?
electrostatics mathematical-physics potential classical-electrodynamics equilibrium
$endgroup$
add a comment |
$begingroup$
Consider a one-dimensional situation on a straight line (say, $x$-axis). Let a charge of magnitude $q$ be located at $x=x_0$, the potential satisfies the Poisson's equation $$fracd^2Vdx^2=-fracrho(x)epsilon_0=-fracqdelta(x-x_0)epsilon_0.$$ If $q>0$, $V^primeprime(x_0)<0$, and if $q<0$, $V^primeprime(x_0)>0$. Therefore, it appears that the potential $V$ does have a minimum at $x=x_0$, for $q<0$. Does this imply that $x=x_0$ is a point of stable equilibrium? I must be missing something because this appears to violate Earnshaw's theorem (or it doesn't)?
electrostatics mathematical-physics potential classical-electrodynamics equilibrium
$endgroup$
add a comment |
$begingroup$
Consider a one-dimensional situation on a straight line (say, $x$-axis). Let a charge of magnitude $q$ be located at $x=x_0$, the potential satisfies the Poisson's equation $$fracd^2Vdx^2=-fracrho(x)epsilon_0=-fracqdelta(x-x_0)epsilon_0.$$ If $q>0$, $V^primeprime(x_0)<0$, and if $q<0$, $V^primeprime(x_0)>0$. Therefore, it appears that the potential $V$ does have a minimum at $x=x_0$, for $q<0$. Does this imply that $x=x_0$ is a point of stable equilibrium? I must be missing something because this appears to violate Earnshaw's theorem (or it doesn't)?
electrostatics mathematical-physics potential classical-electrodynamics equilibrium
$endgroup$
Consider a one-dimensional situation on a straight line (say, $x$-axis). Let a charge of magnitude $q$ be located at $x=x_0$, the potential satisfies the Poisson's equation $$fracd^2Vdx^2=-fracrho(x)epsilon_0=-fracqdelta(x-x_0)epsilon_0.$$ If $q>0$, $V^primeprime(x_0)<0$, and if $q<0$, $V^primeprime(x_0)>0$. Therefore, it appears that the potential $V$ does have a minimum at $x=x_0$, for $q<0$. Does this imply that $x=x_0$ is a point of stable equilibrium? I must be missing something because this appears to violate Earnshaw's theorem (or it doesn't)?
electrostatics mathematical-physics potential classical-electrodynamics equilibrium
electrostatics mathematical-physics potential classical-electrodynamics equilibrium
edited 9 hours ago
Aaron Stevens
14.2k42252
14.2k42252
asked 12 hours ago
SRSSRS
6,513433123
6,513433123
add a comment |
add a comment |
2 Answers
2
active
oldest
votes
$begingroup$
Your example does not contradict Earnshaw's theorem for electrostatics, because it rules out stable equilibrium in a region without charge, possibly containing fields made by charges outside that region. Here you're doing the exact opposite, looking at the only point in your situation with charge.
$endgroup$
$begingroup$
Yes. I meant Earnshaw's theorem. Thanks. Does it mean that there must be an Earnshaw's theorem for Newtonian gravitation? Because in a massless region, again one has $V^primeprime(x)=0$?
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS Yes, that's true.
$endgroup$
– knzhou
11 hours ago
$begingroup$
I am not yet totally comfortable with this. If you have a charge at some point $x=x_0$, is it not correct to look at the behaviour of the potential at that point? @knzhou
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS The potential at a point charge is not defined (or you could say infinite)
$endgroup$
– Aaron Stevens
10 hours ago
$begingroup$
I have to think more about it and I'll get back.
$endgroup$
– SRS
10 hours ago
|
show 1 more comment
$begingroup$
So technically $V''(x_0)$ doesn't have an actual value, since $delta(x-x_0)toinfty$ as $xto x_0$. However, if you understand the Dirac delta distribution to be a limit of a function whose peak "gets narrower" with its integral remaining constant, then this is fine and you could say there is a minimum at $x_0$ for $q<0$
This can be more easily understood by just thinking about the motion of a positive charge in this potential. It will move towards the negative charge, i.e. towards the minimum of the potential.
$endgroup$
add a comment |
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2 Answers
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active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
Your example does not contradict Earnshaw's theorem for electrostatics, because it rules out stable equilibrium in a region without charge, possibly containing fields made by charges outside that region. Here you're doing the exact opposite, looking at the only point in your situation with charge.
$endgroup$
$begingroup$
Yes. I meant Earnshaw's theorem. Thanks. Does it mean that there must be an Earnshaw's theorem for Newtonian gravitation? Because in a massless region, again one has $V^primeprime(x)=0$?
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS Yes, that's true.
$endgroup$
– knzhou
11 hours ago
$begingroup$
I am not yet totally comfortable with this. If you have a charge at some point $x=x_0$, is it not correct to look at the behaviour of the potential at that point? @knzhou
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS The potential at a point charge is not defined (or you could say infinite)
$endgroup$
– Aaron Stevens
10 hours ago
$begingroup$
I have to think more about it and I'll get back.
$endgroup$
– SRS
10 hours ago
|
show 1 more comment
$begingroup$
Your example does not contradict Earnshaw's theorem for electrostatics, because it rules out stable equilibrium in a region without charge, possibly containing fields made by charges outside that region. Here you're doing the exact opposite, looking at the only point in your situation with charge.
$endgroup$
$begingroup$
Yes. I meant Earnshaw's theorem. Thanks. Does it mean that there must be an Earnshaw's theorem for Newtonian gravitation? Because in a massless region, again one has $V^primeprime(x)=0$?
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS Yes, that's true.
$endgroup$
– knzhou
11 hours ago
$begingroup$
I am not yet totally comfortable with this. If you have a charge at some point $x=x_0$, is it not correct to look at the behaviour of the potential at that point? @knzhou
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS The potential at a point charge is not defined (or you could say infinite)
$endgroup$
– Aaron Stevens
10 hours ago
$begingroup$
I have to think more about it and I'll get back.
$endgroup$
– SRS
10 hours ago
|
show 1 more comment
$begingroup$
Your example does not contradict Earnshaw's theorem for electrostatics, because it rules out stable equilibrium in a region without charge, possibly containing fields made by charges outside that region. Here you're doing the exact opposite, looking at the only point in your situation with charge.
$endgroup$
Your example does not contradict Earnshaw's theorem for electrostatics, because it rules out stable equilibrium in a region without charge, possibly containing fields made by charges outside that region. Here you're doing the exact opposite, looking at the only point in your situation with charge.
edited 9 hours ago
Aaron Stevens
14.2k42252
14.2k42252
answered 12 hours ago
knzhouknzhou
46.2k11124223
46.2k11124223
$begingroup$
Yes. I meant Earnshaw's theorem. Thanks. Does it mean that there must be an Earnshaw's theorem for Newtonian gravitation? Because in a massless region, again one has $V^primeprime(x)=0$?
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS Yes, that's true.
$endgroup$
– knzhou
11 hours ago
$begingroup$
I am not yet totally comfortable with this. If you have a charge at some point $x=x_0$, is it not correct to look at the behaviour of the potential at that point? @knzhou
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS The potential at a point charge is not defined (or you could say infinite)
$endgroup$
– Aaron Stevens
10 hours ago
$begingroup$
I have to think more about it and I'll get back.
$endgroup$
– SRS
10 hours ago
|
show 1 more comment
$begingroup$
Yes. I meant Earnshaw's theorem. Thanks. Does it mean that there must be an Earnshaw's theorem for Newtonian gravitation? Because in a massless region, again one has $V^primeprime(x)=0$?
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS Yes, that's true.
$endgroup$
– knzhou
11 hours ago
$begingroup$
I am not yet totally comfortable with this. If you have a charge at some point $x=x_0$, is it not correct to look at the behaviour of the potential at that point? @knzhou
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS The potential at a point charge is not defined (or you could say infinite)
$endgroup$
– Aaron Stevens
10 hours ago
$begingroup$
I have to think more about it and I'll get back.
$endgroup$
– SRS
10 hours ago
$begingroup$
Yes. I meant Earnshaw's theorem. Thanks. Does it mean that there must be an Earnshaw's theorem for Newtonian gravitation? Because in a massless region, again one has $V^primeprime(x)=0$?
$endgroup$
– SRS
11 hours ago
$begingroup$
Yes. I meant Earnshaw's theorem. Thanks. Does it mean that there must be an Earnshaw's theorem for Newtonian gravitation? Because in a massless region, again one has $V^primeprime(x)=0$?
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS Yes, that's true.
$endgroup$
– knzhou
11 hours ago
$begingroup$
@SRS Yes, that's true.
$endgroup$
– knzhou
11 hours ago
$begingroup$
I am not yet totally comfortable with this. If you have a charge at some point $x=x_0$, is it not correct to look at the behaviour of the potential at that point? @knzhou
$endgroup$
– SRS
11 hours ago
$begingroup$
I am not yet totally comfortable with this. If you have a charge at some point $x=x_0$, is it not correct to look at the behaviour of the potential at that point? @knzhou
$endgroup$
– SRS
11 hours ago
$begingroup$
@SRS The potential at a point charge is not defined (or you could say infinite)
$endgroup$
– Aaron Stevens
10 hours ago
$begingroup$
@SRS The potential at a point charge is not defined (or you could say infinite)
$endgroup$
– Aaron Stevens
10 hours ago
$begingroup$
I have to think more about it and I'll get back.
$endgroup$
– SRS
10 hours ago
$begingroup$
I have to think more about it and I'll get back.
$endgroup$
– SRS
10 hours ago
|
show 1 more comment
$begingroup$
So technically $V''(x_0)$ doesn't have an actual value, since $delta(x-x_0)toinfty$ as $xto x_0$. However, if you understand the Dirac delta distribution to be a limit of a function whose peak "gets narrower" with its integral remaining constant, then this is fine and you could say there is a minimum at $x_0$ for $q<0$
This can be more easily understood by just thinking about the motion of a positive charge in this potential. It will move towards the negative charge, i.e. towards the minimum of the potential.
$endgroup$
add a comment |
$begingroup$
So technically $V''(x_0)$ doesn't have an actual value, since $delta(x-x_0)toinfty$ as $xto x_0$. However, if you understand the Dirac delta distribution to be a limit of a function whose peak "gets narrower" with its integral remaining constant, then this is fine and you could say there is a minimum at $x_0$ for $q<0$
This can be more easily understood by just thinking about the motion of a positive charge in this potential. It will move towards the negative charge, i.e. towards the minimum of the potential.
$endgroup$
add a comment |
$begingroup$
So technically $V''(x_0)$ doesn't have an actual value, since $delta(x-x_0)toinfty$ as $xto x_0$. However, if you understand the Dirac delta distribution to be a limit of a function whose peak "gets narrower" with its integral remaining constant, then this is fine and you could say there is a minimum at $x_0$ for $q<0$
This can be more easily understood by just thinking about the motion of a positive charge in this potential. It will move towards the negative charge, i.e. towards the minimum of the potential.
$endgroup$
So technically $V''(x_0)$ doesn't have an actual value, since $delta(x-x_0)toinfty$ as $xto x_0$. However, if you understand the Dirac delta distribution to be a limit of a function whose peak "gets narrower" with its integral remaining constant, then this is fine and you could say there is a minimum at $x_0$ for $q<0$
This can be more easily understood by just thinking about the motion of a positive charge in this potential. It will move towards the negative charge, i.e. towards the minimum of the potential.
answered 12 hours ago
Aaron StevensAaron Stevens
14.2k42252
14.2k42252
add a comment |
add a comment |
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