Prove that $frac{d}{dr}frac{1}{4 pi r^2} iint_{S_r} u dS = frac{1}{4 pi r^2} iint_{S_r} nabla u cdot dvec{S}$











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How can I show that if $u$ is a $C^1$ function and $S_r = {(x, y, z) : x^2 + y^2 + z^2 = r}$, then for all $r$:



$$frac{d}{dr}frac{1}{4 pi r^2} iint_{S_r} u dS = frac{1}{4 pi r^2} iint_{S_r} nabla u cdot dvec{S}$$










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    How can I show that if $u$ is a $C^1$ function and $S_r = {(x, y, z) : x^2 + y^2 + z^2 = r}$, then for all $r$:



    $$frac{d}{dr}frac{1}{4 pi r^2} iint_{S_r} u dS = frac{1}{4 pi r^2} iint_{S_r} nabla u cdot dvec{S}$$










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      How can I show that if $u$ is a $C^1$ function and $S_r = {(x, y, z) : x^2 + y^2 + z^2 = r}$, then for all $r$:



      $$frac{d}{dr}frac{1}{4 pi r^2} iint_{S_r} u dS = frac{1}{4 pi r^2} iint_{S_r} nabla u cdot dvec{S}$$










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      How can I show that if $u$ is a $C^1$ function and $S_r = {(x, y, z) : x^2 + y^2 + z^2 = r}$, then for all $r$:



      $$frac{d}{dr}frac{1}{4 pi r^2} iint_{S_r} u dS = frac{1}{4 pi r^2} iint_{S_r} nabla u cdot dvec{S}$$







      multivariable-calculus






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      asked Nov 19 at 18:58









      John

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          Get the "$r$" out of the limits of integration. With the substitution $rz = y$ you have
          $r^2 dS(u) = dS(y)$ so that $$frac 1{4pi r^2} iint_{S_r} u(y) , dS(y) = frac 1{4pi} iint_{S_1} u(rz) , dS(z) = frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z).$$
          The derivative is calculated using the chain rule:
          $$frac{d}{dr} u(rz_1,rz_2) = frac{partial u}{partial z_1}u(rz_1,rz_2) z_1 + frac{partial u}{partial z_2} u(rz_1,rz_2) z_2 = nabla u(rz_1,rz_2) cdot (z_1,z_2) = nabla u(rz) cdot z.$$ Re-apply the substitution $rz = y$ to obtain
          $$ frac{d}{dr} frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z) = frac 1{4pi} iint_{S_1} nabla u(rz) cdot z , dS(z) = frac 1{4pi r^2} iint_{S_r} nabla u(y) cdot frac yr , dS(y)$$



          Finally observe that the exterior unit normal vector to the sphere $S_r$ at a point $y in S_r$ is just $dfrac yr$.






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            1 Answer
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            1 Answer
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            active

            oldest

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            active

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            active

            oldest

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            up vote
            0
            down vote



            accepted










            Get the "$r$" out of the limits of integration. With the substitution $rz = y$ you have
            $r^2 dS(u) = dS(y)$ so that $$frac 1{4pi r^2} iint_{S_r} u(y) , dS(y) = frac 1{4pi} iint_{S_1} u(rz) , dS(z) = frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z).$$
            The derivative is calculated using the chain rule:
            $$frac{d}{dr} u(rz_1,rz_2) = frac{partial u}{partial z_1}u(rz_1,rz_2) z_1 + frac{partial u}{partial z_2} u(rz_1,rz_2) z_2 = nabla u(rz_1,rz_2) cdot (z_1,z_2) = nabla u(rz) cdot z.$$ Re-apply the substitution $rz = y$ to obtain
            $$ frac{d}{dr} frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z) = frac 1{4pi} iint_{S_1} nabla u(rz) cdot z , dS(z) = frac 1{4pi r^2} iint_{S_r} nabla u(y) cdot frac yr , dS(y)$$



            Finally observe that the exterior unit normal vector to the sphere $S_r$ at a point $y in S_r$ is just $dfrac yr$.






            share|cite|improve this answer

























              up vote
              0
              down vote



              accepted










              Get the "$r$" out of the limits of integration. With the substitution $rz = y$ you have
              $r^2 dS(u) = dS(y)$ so that $$frac 1{4pi r^2} iint_{S_r} u(y) , dS(y) = frac 1{4pi} iint_{S_1} u(rz) , dS(z) = frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z).$$
              The derivative is calculated using the chain rule:
              $$frac{d}{dr} u(rz_1,rz_2) = frac{partial u}{partial z_1}u(rz_1,rz_2) z_1 + frac{partial u}{partial z_2} u(rz_1,rz_2) z_2 = nabla u(rz_1,rz_2) cdot (z_1,z_2) = nabla u(rz) cdot z.$$ Re-apply the substitution $rz = y$ to obtain
              $$ frac{d}{dr} frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z) = frac 1{4pi} iint_{S_1} nabla u(rz) cdot z , dS(z) = frac 1{4pi r^2} iint_{S_r} nabla u(y) cdot frac yr , dS(y)$$



              Finally observe that the exterior unit normal vector to the sphere $S_r$ at a point $y in S_r$ is just $dfrac yr$.






              share|cite|improve this answer























                up vote
                0
                down vote



                accepted







                up vote
                0
                down vote



                accepted






                Get the "$r$" out of the limits of integration. With the substitution $rz = y$ you have
                $r^2 dS(u) = dS(y)$ so that $$frac 1{4pi r^2} iint_{S_r} u(y) , dS(y) = frac 1{4pi} iint_{S_1} u(rz) , dS(z) = frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z).$$
                The derivative is calculated using the chain rule:
                $$frac{d}{dr} u(rz_1,rz_2) = frac{partial u}{partial z_1}u(rz_1,rz_2) z_1 + frac{partial u}{partial z_2} u(rz_1,rz_2) z_2 = nabla u(rz_1,rz_2) cdot (z_1,z_2) = nabla u(rz) cdot z.$$ Re-apply the substitution $rz = y$ to obtain
                $$ frac{d}{dr} frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z) = frac 1{4pi} iint_{S_1} nabla u(rz) cdot z , dS(z) = frac 1{4pi r^2} iint_{S_r} nabla u(y) cdot frac yr , dS(y)$$



                Finally observe that the exterior unit normal vector to the sphere $S_r$ at a point $y in S_r$ is just $dfrac yr$.






                share|cite|improve this answer












                Get the "$r$" out of the limits of integration. With the substitution $rz = y$ you have
                $r^2 dS(u) = dS(y)$ so that $$frac 1{4pi r^2} iint_{S_r} u(y) , dS(y) = frac 1{4pi} iint_{S_1} u(rz) , dS(z) = frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z).$$
                The derivative is calculated using the chain rule:
                $$frac{d}{dr} u(rz_1,rz_2) = frac{partial u}{partial z_1}u(rz_1,rz_2) z_1 + frac{partial u}{partial z_2} u(rz_1,rz_2) z_2 = nabla u(rz_1,rz_2) cdot (z_1,z_2) = nabla u(rz) cdot z.$$ Re-apply the substitution $rz = y$ to obtain
                $$ frac{d}{dr} frac 1{4pi} iint_{S_1} u(rz_1,rz_2) , dS(z) = frac 1{4pi} iint_{S_1} nabla u(rz) cdot z , dS(z) = frac 1{4pi r^2} iint_{S_r} nabla u(y) cdot frac yr , dS(y)$$



                Finally observe that the exterior unit normal vector to the sphere $S_r$ at a point $y in S_r$ is just $dfrac yr$.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Nov 19 at 21:05









                Umberto P.

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                38.3k13063






























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