If $u$ is harmonic and vanishes on the boundary, then $uequiv 0$.
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Let's assume $u$ is harmonic on $D=x^2+y^2leq1$. If $u=0$ on $partial D$ then $uequiv 0$ on $D$.
$textbfProof$:
Let's use Green's theorem and set $P=-ufracpartial upartial y$ and $Q=ufracpartial upartial x$.
Then
$$1. fracpartial Qpartial x-fracpartial Ppartial y
=left(fracpartial upartial xright)^2+
uleft(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2+
uleft(fracpartial upartial yright)^2
=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2.
$$
By Green's theorem,
$$
0=int_partial D -ufracpartial upartial ydx+ufracpartial upartial xdy=int int_D
left(
left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2right)dxdy.
$$
Because $uin C^2$, we get
$$
left(fracpartial upartial xright)^2 +
left(fracpartial upartial yright)^2=0.
$$
So $uequiv c$ on $D$ but on $partial D$ we have $u=0$. So $uequiv 0$.
What have we done on the first move for $1$.?
calculus analysis
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up vote
1
down vote
favorite
Let's assume $u$ is harmonic on $D=x^2+y^2leq1$. If $u=0$ on $partial D$ then $uequiv 0$ on $D$.
$textbfProof$:
Let's use Green's theorem and set $P=-ufracpartial upartial y$ and $Q=ufracpartial upartial x$.
Then
$$1. fracpartial Qpartial x-fracpartial Ppartial y
=left(fracpartial upartial xright)^2+
uleft(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2+
uleft(fracpartial upartial yright)^2
=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2.
$$
By Green's theorem,
$$
0=int_partial D -ufracpartial upartial ydx+ufracpartial upartial xdy=int int_D
left(
left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2right)dxdy.
$$
Because $uin C^2$, we get
$$
left(fracpartial upartial xright)^2 +
left(fracpartial upartial yright)^2=0.
$$
So $uequiv c$ on $D$ but on $partial D$ we have $u=0$. So $uequiv 0$.
What have we done on the first move for $1$.?
calculus analysis
You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
– Raymond Chu
Jul 29 at 17:06
add a comment |Â
up vote
1
down vote
favorite
up vote
1
down vote
favorite
Let's assume $u$ is harmonic on $D=x^2+y^2leq1$. If $u=0$ on $partial D$ then $uequiv 0$ on $D$.
$textbfProof$:
Let's use Green's theorem and set $P=-ufracpartial upartial y$ and $Q=ufracpartial upartial x$.
Then
$$1. fracpartial Qpartial x-fracpartial Ppartial y
=left(fracpartial upartial xright)^2+
uleft(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2+
uleft(fracpartial upartial yright)^2
=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2.
$$
By Green's theorem,
$$
0=int_partial D -ufracpartial upartial ydx+ufracpartial upartial xdy=int int_D
left(
left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2right)dxdy.
$$
Because $uin C^2$, we get
$$
left(fracpartial upartial xright)^2 +
left(fracpartial upartial yright)^2=0.
$$
So $uequiv c$ on $D$ but on $partial D$ we have $u=0$. So $uequiv 0$.
What have we done on the first move for $1$.?
calculus analysis
Let's assume $u$ is harmonic on $D=x^2+y^2leq1$. If $u=0$ on $partial D$ then $uequiv 0$ on $D$.
$textbfProof$:
Let's use Green's theorem and set $P=-ufracpartial upartial y$ and $Q=ufracpartial upartial x$.
Then
$$1. fracpartial Qpartial x-fracpartial Ppartial y
=left(fracpartial upartial xright)^2+
uleft(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2+
uleft(fracpartial upartial yright)^2
=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2.
$$
By Green's theorem,
$$
0=int_partial D -ufracpartial upartial ydx+ufracpartial upartial xdy=int int_D
left(
left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2right)dxdy.
$$
Because $uin C^2$, we get
$$
left(fracpartial upartial xright)^2 +
left(fracpartial upartial yright)^2=0.
$$
So $uequiv c$ on $D$ but on $partial D$ we have $u=0$. So $uequiv 0$.
What have we done on the first move for $1$.?
calculus analysis
edited Jul 29 at 16:26
Mee Seong Im
2,5591517
2,5591517
asked Jul 29 at 15:02
newhere
742310
742310
You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
– Raymond Chu
Jul 29 at 17:06
add a comment |Â
You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
– Raymond Chu
Jul 29 at 17:06
You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
– Raymond Chu
Jul 29 at 17:06
You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
– Raymond Chu
Jul 29 at 17:06
add a comment |Â
2 Answers
2
active
oldest
votes
up vote
1
down vote
accepted
In the second line of your proof, it should be:
beginalign*
fracpartial Qpartial x-fracpartial Ppartial y
&=left(fracpartial upartial xright)^2+
ufracpartial^2 upartial x^2+
left(fracpartial upartial yright)^2+
u fracpartial^2 upartial y^2 \
&= left(fracpartial upartial xright)^2
+ left(fracpartial upartial yright)^2
+ u
underbraceleft( fracpartial^2 upartial x^2
+ fracpartial^2 upartial y^2right)_0 \
&=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2
endalign*
since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.
add a comment |Â
up vote
1
down vote
We have used the product rule; e.g.
$$
partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
$$
(Your notation seems a bit off at that point.)
Is the sentence true only on a circle?
– newhere
Jul 29 at 15:38
In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
– AlgebraicsAnonymous
Jul 29 at 15:39
add a comment |Â
2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
1
down vote
accepted
In the second line of your proof, it should be:
beginalign*
fracpartial Qpartial x-fracpartial Ppartial y
&=left(fracpartial upartial xright)^2+
ufracpartial^2 upartial x^2+
left(fracpartial upartial yright)^2+
u fracpartial^2 upartial y^2 \
&= left(fracpartial upartial xright)^2
+ left(fracpartial upartial yright)^2
+ u
underbraceleft( fracpartial^2 upartial x^2
+ fracpartial^2 upartial y^2right)_0 \
&=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2
endalign*
since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.
add a comment |Â
up vote
1
down vote
accepted
In the second line of your proof, it should be:
beginalign*
fracpartial Qpartial x-fracpartial Ppartial y
&=left(fracpartial upartial xright)^2+
ufracpartial^2 upartial x^2+
left(fracpartial upartial yright)^2+
u fracpartial^2 upartial y^2 \
&= left(fracpartial upartial xright)^2
+ left(fracpartial upartial yright)^2
+ u
underbraceleft( fracpartial^2 upartial x^2
+ fracpartial^2 upartial y^2right)_0 \
&=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2
endalign*
since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.
add a comment |Â
up vote
1
down vote
accepted
up vote
1
down vote
accepted
In the second line of your proof, it should be:
beginalign*
fracpartial Qpartial x-fracpartial Ppartial y
&=left(fracpartial upartial xright)^2+
ufracpartial^2 upartial x^2+
left(fracpartial upartial yright)^2+
u fracpartial^2 upartial y^2 \
&= left(fracpartial upartial xright)^2
+ left(fracpartial upartial yright)^2
+ u
underbraceleft( fracpartial^2 upartial x^2
+ fracpartial^2 upartial y^2right)_0 \
&=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2
endalign*
since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.
In the second line of your proof, it should be:
beginalign*
fracpartial Qpartial x-fracpartial Ppartial y
&=left(fracpartial upartial xright)^2+
ufracpartial^2 upartial x^2+
left(fracpartial upartial yright)^2+
u fracpartial^2 upartial y^2 \
&= left(fracpartial upartial xright)^2
+ left(fracpartial upartial yright)^2
+ u
underbraceleft( fracpartial^2 upartial x^2
+ fracpartial^2 upartial y^2right)_0 \
&=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2
endalign*
since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.
answered Jul 29 at 16:45
Mee Seong Im
2,5591517
2,5591517
add a comment |Â
add a comment |Â
up vote
1
down vote
We have used the product rule; e.g.
$$
partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
$$
(Your notation seems a bit off at that point.)
Is the sentence true only on a circle?
– newhere
Jul 29 at 15:38
In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
– AlgebraicsAnonymous
Jul 29 at 15:39
add a comment |Â
up vote
1
down vote
We have used the product rule; e.g.
$$
partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
$$
(Your notation seems a bit off at that point.)
Is the sentence true only on a circle?
– newhere
Jul 29 at 15:38
In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
– AlgebraicsAnonymous
Jul 29 at 15:39
add a comment |Â
up vote
1
down vote
up vote
1
down vote
We have used the product rule; e.g.
$$
partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
$$
(Your notation seems a bit off at that point.)
We have used the product rule; e.g.
$$
partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
$$
(Your notation seems a bit off at that point.)
answered Jul 29 at 15:30
AlgebraicsAnonymous
66611
66611
Is the sentence true only on a circle?
– newhere
Jul 29 at 15:38
In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
– AlgebraicsAnonymous
Jul 29 at 15:39
add a comment |Â
Is the sentence true only on a circle?
– newhere
Jul 29 at 15:38
In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
– AlgebraicsAnonymous
Jul 29 at 15:39
Is the sentence true only on a circle?
– newhere
Jul 29 at 15:38
Is the sentence true only on a circle?
– newhere
Jul 29 at 15:38
In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
– AlgebraicsAnonymous
Jul 29 at 15:39
In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
– AlgebraicsAnonymous
Jul 29 at 15:39
add a comment |Â
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You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
– Raymond Chu
Jul 29 at 17:06