Surface integrals of vector fields, normal - does scaling matter?

  • #1
laser1
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13
Homework Statement
desc
Relevant Equations
N.A.
1729765210106.png

Source: https://tutorial.math.lamar.edu/Problems/CalcIII/SurfIntVectorField.aspx

Alright so my confusion lies in the following step: Consider the side x = 0. Okay, from the formula (I am just going to insert an image here)

WhatsApp Image 2024-10-24 at 11.23.22.jpeg

Okay, so gradient of f would just be <1, 0, 0>, which is simply i, which agrees with the solution. However, what if I said that the plane x = 0 is equivalent to the plane 2x = 0? Then the gradient would be <2, 0, 0>, which changes the problem! There must be a flaw in my logic here, but I can't figure it out. Thanks!
 
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  • #2
The plane [itex]kx = 0[/itex] has surface element [itex]dy\,dz[/itex]. Its unit normal is [itex]\pm \mathbf{e}_x[/itex], so [itex]d\mathbf{S} = \pm\mathbf{e}_x\,dy\,dz[/itex].

What appears in your image implies [itex]dS = \|\nabla f\|\,dA[/itex], which is a change of variable from [itex](y,z)[/itex] to something different. Working out the detail there should cancel the 2 you introduced into [itex]\nabla f = 2\mathbf{e}_x[/itex].
 
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  • #3
pasmith said:
What appears in your image implies [itex]dS = \|\nabla f\|\,dA[/itex]
Oh, is this not correct then? Edit: I am not fully sure what you are saying
 
  • #4
The normal of a level surface of [itex]f[/itex] is parallel to [itex]\nabla f[/itex], ie. there is some non-zero scalar field [itex]k[/itex] such that [tex]
\frac{\partial \mathbf{r}}{\partial u} \times \frac{\partial \mathbf{r}}{\partial v} = k(u,v)\nabla f[/tex] so that [tex]
d\mathbf{S} = \frac{\partial \mathbf{r}}{\partial u} \times \frac{\partial \mathbf{r}}{\partial v}\,du\,dv =
k \nabla f \,du\,dv[/tex] and [tex]dS = |k|\|\nabla f\|\,du\,dv.[/tex] The actual source of your error is to assume [itex]k \equiv 1[/itex].

If you parametrize [itex]f(x,y,z) = Cx = 0[/itex], [itex]C \neq 0[/itex], as [itex]\mathbf{r}(u,v) = u\mathbf{e}_y + v\mathbf{e}_z[/itex] then you find [tex]d\mathbf{S} =
\frac{\partial \mathbf{r}}{\partial u} \times \frac{\partial \mathbf{r}}{\partial v}\,du\,dv = \mathbf{e}_y \times \mathbf{e}_z\,du\,dv = \mathbf{e}_x\,du\,dv = \frac1C \nabla f\,du\,dv[/tex] so that [itex]k \equiv \frac1C[/itex].
 
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  • #5
pasmith said:
The normal of a level surface of [itex]f[/itex] is parallel to [itex]\nabla f[/itex], ie. there is some non-zero scalar field [itex]k[/itex] such that [tex]
\frac{\partial \mathbf{r}}{\partial u} \times \frac{\partial \mathbf{r}}{\partial v} = k(u,v)\nabla f[/tex] so that [tex]
d\mathbf{S} = \frac{\partial \mathbf{r}}{\partial u} \times \frac{\partial \mathbf{r}}{\partial v}\,du\,dv =
k \nabla f \,du\,dv[/tex] and [tex]dS = |k|\|\nabla f\|\,du\,dv.[/tex] The actual source of your error is to assume [itex]k \equiv 1[/itex].

If you parametrize [itex]f(x,y,z) = Cx = 0[/itex], [itex]C \neq 0[/itex], as [itex]\mathbf{r}(u,v) = u\mathbf{e}_y + v\mathbf{e}_z[/itex] then you find [tex]d\mathbf{S} =
\frac{\partial \mathbf{r}}{\partial u} \times \frac{\partial \mathbf{r}}{\partial v}\,du\,dv = \mathbf{e}_y \times \mathbf{e}_z\,du\,dv = \mathbf{e}_x\,du\,dv = \frac1C \nabla f\,du\,dv[/tex] so that [itex]k \equiv \frac1C[/itex].
Thanks, that makes sense! What about this other example?
1729852873593.png

It seems equally as valid to parameterise a surface as <0, 2y, 2z>, where y and z can be any number, to represent x = 0. Yet the results suggest otherwise!
 
  • #6
The general case for [itex]f(x,y,z) = x = 0[/itex] is [itex]\mathbf{r} = y(u,v)\mathbf{e}_y + z(y,v)\mathbf{e}_z[/itex], with [tex]
d\mathbf{S} = \mathbf{e}_x \left( \frac{\partial y}{\partial u}\frac{\partial z}{\partial v} - \frac{\partial z}{\partial u}\frac{\partial y}{\partial v}\right)\,du\,dv[/tex] and [tex]
dS = \left| \frac{\partial y}{\partial u}\frac{\partial z}{\partial v} - \frac{\partial z}{\partial u}\frac{\partial y}{\partial v} \right|\,du\,dv[/tex] which you should recognise as the change of variable formula for a double integral, [tex]
dy\,dz = \left| \frac{\partial y}{\partial u}\frac{\partial z}{\partial v} - \frac{\partial z}{\partial u}\frac{\partial y}{\partial v} \right|\,du\,dv.[/tex]
 
  • #7
pasmith said:
The general case for [itex]f(x,y,z) = x = 0[/itex] is [itex]\mathbf{r} = y(u,v)\mathbf{e}_y + z(y,v)\mathbf{e}_z[/itex], with [tex]
d\mathbf{S} = \mathbf{e}_x \left( \frac{\partial y}{\partial u}\frac{\partial z}{\partial v} - \frac{\partial z}{\partial u}\frac{\partial y}{\partial v}\right)\,du\,dv[/tex] and [tex]
dS = \left| \frac{\partial y}{\partial u}\frac{\partial z}{\partial v} - \frac{\partial z}{\partial u}\frac{\partial y}{\partial v} \right|\,du\,dv[/tex] which you should recognise as the change of variable formula for a double integral, [tex]
dy\,dz = \left| \frac{\partial y}{\partial u}\frac{\partial z}{\partial v} - \frac{\partial z}{\partial u}\frac{\partial y}{\partial v} \right|\,du\,dv.[/tex]
I don't follow, sorry. In one example I get ##\textbf{i}## and in the other example I get ##\textbf{4i}## for the same equation.
 
  • #8
laser1 said:
I don't follow, sorry. In one example I get ##\textbf{i}## and in the other example I get ##\textbf{4i}## for the same equation.
resolved: the parameterisation is different, so the bounds will change accordingly. All is fine! :)
 

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