Prove that this $ langle u,vrangle = int_Omega [ bigtriangledown u cdotbigtriangledown v +uv ] $ is an inner...












0












$begingroup$


Information needed



$$I = (a,b)$$



$$ H_0^1 (I) = { v in H^1(I) : v(a)= v(b) = 0 } $$



$$ H^1 (I) = { v: v , v' in mathbb{L}_2(I) } $$



$$ mathbb{L}_2(I) = { v:v text{ it's defined at } I text{ and } int v^2,dx < infty } $$



Prove that this is a scalar product in $H^1_0 $



Using the notation $$ langle u,vrangle = int_Omega [ bigtriangledown u cdotbigtriangledown v +uv ] $$



where $Omega$ is a bounded domain.



In the book numerical solutions of PDE by the finite element method by Claes there is this passage and I could not see clearly this statement.



Thanks to any help !










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$endgroup$








  • 3




    $begingroup$
    Have you tried proving it yourself? An inner product has three defining properties, each of which should not be too hard to verify.
    $endgroup$
    – MaoWao
    Jan 30 at 12:15










  • $begingroup$
    you mean, symmetry; linearity and podsitive definiteness ?
    $endgroup$
    – Saiten
    Jan 30 at 12:19










  • $begingroup$
    It's bilinearity (linearity in each argument separately), not linearity. Otherwise yes.
    $endgroup$
    – MaoWao
    Jan 30 at 12:23










  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 12:39










  • $begingroup$
    Thankss for the help!
    $endgroup$
    – Saiten
    Jan 30 at 13:24
















0












$begingroup$


Information needed



$$I = (a,b)$$



$$ H_0^1 (I) = { v in H^1(I) : v(a)= v(b) = 0 } $$



$$ H^1 (I) = { v: v , v' in mathbb{L}_2(I) } $$



$$ mathbb{L}_2(I) = { v:v text{ it's defined at } I text{ and } int v^2,dx < infty } $$



Prove that this is a scalar product in $H^1_0 $



Using the notation $$ langle u,vrangle = int_Omega [ bigtriangledown u cdotbigtriangledown v +uv ] $$



where $Omega$ is a bounded domain.



In the book numerical solutions of PDE by the finite element method by Claes there is this passage and I could not see clearly this statement.



Thanks to any help !










share|cite|improve this question











$endgroup$








  • 3




    $begingroup$
    Have you tried proving it yourself? An inner product has three defining properties, each of which should not be too hard to verify.
    $endgroup$
    – MaoWao
    Jan 30 at 12:15










  • $begingroup$
    you mean, symmetry; linearity and podsitive definiteness ?
    $endgroup$
    – Saiten
    Jan 30 at 12:19










  • $begingroup$
    It's bilinearity (linearity in each argument separately), not linearity. Otherwise yes.
    $endgroup$
    – MaoWao
    Jan 30 at 12:23










  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 12:39










  • $begingroup$
    Thankss for the help!
    $endgroup$
    – Saiten
    Jan 30 at 13:24














0












0








0





$begingroup$


Information needed



$$I = (a,b)$$



$$ H_0^1 (I) = { v in H^1(I) : v(a)= v(b) = 0 } $$



$$ H^1 (I) = { v: v , v' in mathbb{L}_2(I) } $$



$$ mathbb{L}_2(I) = { v:v text{ it's defined at } I text{ and } int v^2,dx < infty } $$



Prove that this is a scalar product in $H^1_0 $



Using the notation $$ langle u,vrangle = int_Omega [ bigtriangledown u cdotbigtriangledown v +uv ] $$



where $Omega$ is a bounded domain.



In the book numerical solutions of PDE by the finite element method by Claes there is this passage and I could not see clearly this statement.



Thanks to any help !










share|cite|improve this question











$endgroup$




Information needed



$$I = (a,b)$$



$$ H_0^1 (I) = { v in H^1(I) : v(a)= v(b) = 0 } $$



$$ H^1 (I) = { v: v , v' in mathbb{L}_2(I) } $$



$$ mathbb{L}_2(I) = { v:v text{ it's defined at } I text{ and } int v^2,dx < infty } $$



Prove that this is a scalar product in $H^1_0 $



Using the notation $$ langle u,vrangle = int_Omega [ bigtriangledown u cdotbigtriangledown v +uv ] $$



where $Omega$ is a bounded domain.



In the book numerical solutions of PDE by the finite element method by Claes there is this passage and I could not see clearly this statement.



Thanks to any help !







functional-analysis metric-spaces hilbert-spaces






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Jan 30 at 14:32









Adrian Keister

5,26971933




5,26971933










asked Jan 30 at 12:07









SaitenSaiten

346




346








  • 3




    $begingroup$
    Have you tried proving it yourself? An inner product has three defining properties, each of which should not be too hard to verify.
    $endgroup$
    – MaoWao
    Jan 30 at 12:15










  • $begingroup$
    you mean, symmetry; linearity and podsitive definiteness ?
    $endgroup$
    – Saiten
    Jan 30 at 12:19










  • $begingroup$
    It's bilinearity (linearity in each argument separately), not linearity. Otherwise yes.
    $endgroup$
    – MaoWao
    Jan 30 at 12:23










  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 12:39










  • $begingroup$
    Thankss for the help!
    $endgroup$
    – Saiten
    Jan 30 at 13:24














  • 3




    $begingroup$
    Have you tried proving it yourself? An inner product has three defining properties, each of which should not be too hard to verify.
    $endgroup$
    – MaoWao
    Jan 30 at 12:15










  • $begingroup$
    you mean, symmetry; linearity and podsitive definiteness ?
    $endgroup$
    – Saiten
    Jan 30 at 12:19










  • $begingroup$
    It's bilinearity (linearity in each argument separately), not linearity. Otherwise yes.
    $endgroup$
    – MaoWao
    Jan 30 at 12:23










  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 12:39










  • $begingroup$
    Thankss for the help!
    $endgroup$
    – Saiten
    Jan 30 at 13:24








3




3




$begingroup$
Have you tried proving it yourself? An inner product has three defining properties, each of which should not be too hard to verify.
$endgroup$
– MaoWao
Jan 30 at 12:15




$begingroup$
Have you tried proving it yourself? An inner product has three defining properties, each of which should not be too hard to verify.
$endgroup$
– MaoWao
Jan 30 at 12:15












$begingroup$
you mean, symmetry; linearity and podsitive definiteness ?
$endgroup$
– Saiten
Jan 30 at 12:19




$begingroup$
you mean, symmetry; linearity and podsitive definiteness ?
$endgroup$
– Saiten
Jan 30 at 12:19












$begingroup$
It's bilinearity (linearity in each argument separately), not linearity. Otherwise yes.
$endgroup$
– MaoWao
Jan 30 at 12:23




$begingroup$
It's bilinearity (linearity in each argument separately), not linearity. Otherwise yes.
$endgroup$
– MaoWao
Jan 30 at 12:23












$begingroup$
Use $langle Xrangle$ for $langle Xrangle$.
$endgroup$
– Shaun
Jan 30 at 12:39




$begingroup$
Use $langle Xrangle$ for $langle Xrangle$.
$endgroup$
– Shaun
Jan 30 at 12:39












$begingroup$
Thankss for the help!
$endgroup$
– Saiten
Jan 30 at 13:24




$begingroup$
Thankss for the help!
$endgroup$
– Saiten
Jan 30 at 13:24










1 Answer
1






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oldest

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1












$begingroup$

Once you establish that the expression is well defined, you just need to verify the conditions for an inner product.





  1. $langle u,v rangle = langle v,u rangle$.


  2. $langle a u, vrangle = a langle u,brangle$ and $langle u+v,wrangle = langle u,wrangle+langle v,wrangle$.


  3. $langle u,uranglege 0$ and $langle u,urangle=0 Leftrightarrow u = 0$


The third property is the trickiest. You need to show that if $u in H^1_0$ and
$$
int_I (|nabla u|^2 + u^2) = 0
$$

then $u=0$ almost everywhere in $I$.






share|cite|improve this answer











$endgroup$













  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 13:17












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1 Answer
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1 Answer
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active

oldest

votes









active

oldest

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active

oldest

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1












$begingroup$

Once you establish that the expression is well defined, you just need to verify the conditions for an inner product.





  1. $langle u,v rangle = langle v,u rangle$.


  2. $langle a u, vrangle = a langle u,brangle$ and $langle u+v,wrangle = langle u,wrangle+langle v,wrangle$.


  3. $langle u,uranglege 0$ and $langle u,urangle=0 Leftrightarrow u = 0$


The third property is the trickiest. You need to show that if $u in H^1_0$ and
$$
int_I (|nabla u|^2 + u^2) = 0
$$

then $u=0$ almost everywhere in $I$.






share|cite|improve this answer











$endgroup$













  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 13:17
















1












$begingroup$

Once you establish that the expression is well defined, you just need to verify the conditions for an inner product.





  1. $langle u,v rangle = langle v,u rangle$.


  2. $langle a u, vrangle = a langle u,brangle$ and $langle u+v,wrangle = langle u,wrangle+langle v,wrangle$.


  3. $langle u,uranglege 0$ and $langle u,urangle=0 Leftrightarrow u = 0$


The third property is the trickiest. You need to show that if $u in H^1_0$ and
$$
int_I (|nabla u|^2 + u^2) = 0
$$

then $u=0$ almost everywhere in $I$.






share|cite|improve this answer











$endgroup$













  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 13:17














1












1








1





$begingroup$

Once you establish that the expression is well defined, you just need to verify the conditions for an inner product.





  1. $langle u,v rangle = langle v,u rangle$.


  2. $langle a u, vrangle = a langle u,brangle$ and $langle u+v,wrangle = langle u,wrangle+langle v,wrangle$.


  3. $langle u,uranglege 0$ and $langle u,urangle=0 Leftrightarrow u = 0$


The third property is the trickiest. You need to show that if $u in H^1_0$ and
$$
int_I (|nabla u|^2 + u^2) = 0
$$

then $u=0$ almost everywhere in $I$.






share|cite|improve this answer











$endgroup$



Once you establish that the expression is well defined, you just need to verify the conditions for an inner product.





  1. $langle u,v rangle = langle v,u rangle$.


  2. $langle a u, vrangle = a langle u,brangle$ and $langle u+v,wrangle = langle u,wrangle+langle v,wrangle$.


  3. $langle u,uranglege 0$ and $langle u,urangle=0 Leftrightarrow u = 0$


The third property is the trickiest. You need to show that if $u in H^1_0$ and
$$
int_I (|nabla u|^2 + u^2) = 0
$$

then $u=0$ almost everywhere in $I$.







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited Jan 30 at 13:41

























answered Jan 30 at 12:25









PierreCarrePierreCarre

1,734212




1,734212












  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 13:17


















  • $begingroup$
    Use $langle Xrangle$ for $langle Xrangle$.
    $endgroup$
    – Shaun
    Jan 30 at 13:17
















$begingroup$
Use $langle Xrangle$ for $langle Xrangle$.
$endgroup$
– Shaun
Jan 30 at 13:17




$begingroup$
Use $langle Xrangle$ for $langle Xrangle$.
$endgroup$
– Shaun
Jan 30 at 13:17


















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