What are some vector calculus questions about gradient, divergence, and curl?

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Discussion Overview

The discussion revolves around vector calculus concepts, specifically focusing on the gradient, divergence, and curl operators. Participants explore geometric interpretations, evaluate mathematical expressions, and seek clarification on the application of various calculus rules in these contexts.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Homework-related
  • Exploratory

Main Points Raised

  • One participant questions the interpretation of a relation involving the gradient operator and its implications for movement between level surfaces.
  • Another participant discusses the evaluation of the divergence of a vector and seeks clarification on the equivalence of two expressions, suggesting the use of product and chain rules.
  • A different participant challenges the understanding of the gradient's relationship to level surfaces, emphasizing that the gradient is perpendicular to these surfaces.
  • Several participants express confusion regarding the application of the product rule in the context of the curl operator and its simplification.
  • One participant mentions the use of the Leibniz rule to arrive at a solution for the curl of a product of a scalar and a vector field.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and disagreement, particularly regarding the interpretations of the gradient and the application of calculus rules. Some participants provide corrections or alternative perspectives without reaching a consensus.

Contextual Notes

Participants reference specific mathematical steps and rules, such as the product rule and chain rule, but do not fully resolve all expressions or assumptions, leaving some aspects of the discussion open-ended.

Who May Find This Useful

This discussion may be useful for students or individuals studying vector calculus, particularly those seeking clarification on the gradient, divergence, and curl operators and their applications in various contexts.

misogynisticfeminist
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1. I was reading on the geometric interpretation of the grad operator. I've did until the point where this particular relation was given.

[tex]d\varphi=0=C_1-C_1=\Delta C=(\nabla \varphi)\bullet d \vec r[/tex]

This is when we permit [tex]\vec r[/tex] to take us from the surface [tex]\varphi (x,y,z)=C_1[/tex] to another adjacent surface [tex]\varphi (x,y,z)=C_2[/tex] where c are constants.

Why is it that in the first equation we have [tex]C_1-C_1[/tex] ?? Also, why is it that the consequence of the first relation shows that,

for a given [tex]\vert {d\vec r}\vert[/tex], the change of [tex]\varphi[/tex], [tex]d \varphi[/tex] is maximum when [tex]\vert {d\vec r}\vert[/tex] is parellel to [tex]\nabla\varphi[/tex] when [tex]\nabla\varphi[/tex] is normal to the surface.

2. While evaluating the divergence of vector, [tex]\nabla \bullet \vec r f(r) = \frac {\partial}{\partial x} (xf(r))+ \frac {\partial}{\partial y}(yf(r))+ \frac{\partial}{\partial z} (zf(r))[/tex],

why is it equivalent to,

[tex]3 f(r)+\frac {x^2}{r} \frac {df}{dr}+\frac {y^2}{r} \frac {df}{dr}+\frac {z^2}{r} \frac {df}{dr}[/tex] ?

I've tried manipulating the partial differentials using chain rules and all but don't seem to get it. Can someone show me the steps how? Also,

3. I was trying to simplify[tex]\nabla \times f \vec v \vert _x = \frac {\partial}{\partial y} (f V_z)-\frac {\partial}{\partial z} (f V_y)[/tex]. Also, how does it reduce to the final answer,

[tex]f \nabla \times \vec V \vert _x +\nabla f \times \vec V \vert _x[/tex]??

I have also tried manipulating the partial derivatives to no avail. Can someone help? thanks a lot...

: )
 
Last edited:
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misogynisticfeminist said:
2. While evaluating the divergence of vector, [tex]\nabla \bullet \vec r f(r) = \frac {\partial}{\partial x} (xf(r))+ \frac {\partial}{\partial y}(yf(r))+ \frac{\partial}{\partial z} (zf(r))[/tex],

why is it equivalent to,

[tex]3 f(r)+\frac {x^2}{r} \frac {df}{dr}+\frac {y^2}{r} \frac {df}{dr}+\frac {z^2}{r} \frac {df}{dr}[/tex] ?
Here you should use the product and chain rule. Also: [itex]r=\sqrt{x^2+y^2+z^2}[/itex]

So for example:

[tex]\frac{\partial}{\partial x}(xf(r))=f(r)+x\frac{\partial}{\partial x}f(r)[/tex]
This explains where the 3f(r) comes from.
Now:

[tex]\frac{\partial}{\partial x}f(r(x,y,z))=\frac{df}{dr}\frac{\partial r}{\partial x}[/tex]
 
"This is when we permit to take us from the surface [tex]\varphi (x,y,z)=C_1[/tex]
to another adjacent surface [tex]\varphi (x,y,z)=C_1[/tex] where c are constants."

No, I don't think that's what that particular formula is intended to show. What that shows is that the derivative in a direction tangent to a level surface is 0 so [tex](\nabla \varphi)\bullet d \vec r= 0[/tex]: that is, the gradient is perpendicular to all level surfaces.
What is true is that, since [itex]\vec u \bullet \vec v= |\vec u||\vec v|cos(\theta)[/tex], [tex](\nabla \varphi)\bullet d \vec r[/tex] is largest when cos(&theta;) is 1: i.e. &theta;= 0 and the two vectors are parallel.<br /> <br /> For 2, I surprised you didn't see it while looking at the chain rule.<br /> [tex]r= (x^2+ y^2+ z^2)^{\frac{1}{2}}[/tex] so [tex]\frac{\partial r}{\partial x}= \frac{1}{2}(x^2+ y^2+ z^2)^\frac{-1}{2}(2x)= \frac{x}{r}[/tex].<br /> Of course, the same is true of the derivative with respect to y and z.<br /> Now, [tex]\frac{\partial}{\partial x}(xf(r))= f(r)+ x\frac{\partial f}{/partial x}= f(r)+ \frac{x^2 f'(r)}{r}[/tex].<br /> <br /> That first term is what gives you "3f(r)".[/itex]
 
Hey, thanks a lot, that helped. Actually what i had problems with was the use of the product rule while evaluating [tex]\partial/ \ {\partial} x (xf(r))[/tex] and i also failed to keep in mind that [tex]r=\sqrt {x^2+y^2+z^2[/tex] but that was sorted out anyway.

thanks a lot. I've still got one question regarding the curl operator though...hope that someone could help me with that.
 
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In general

[tex](\nabla\times\vec{f})_{x}=...?[/tex]

Daniel.
 
dextercioby said:
In general

[tex](\nabla\times\vec{f})_{x}=...?[/tex]

Daniel.

For, [tex]\nabla \times \vec f[/tex], it is,

[tex]det \left(<br /> \begin{array}{ccc}<br /> <br /> \hat x & \hat y & \hat z\\<br /> {\partial}/{\partial x} & {\partial}/{\partial y} & {\partial}/{\partial z} \\<br /> F_x & F_y & F_z \\<br /> <br /> \end{array}<br /> \right)<br /> [/tex]

(the matrix is quite horrible though, i can't seem to type it the right way, but i guess you know what i mean).

hmmm, I've tried doing the curl again, i got,

[tex]\nabla \times f \vec v \vert _x = \frac {\partial}{\partial y} (f V_z)-\frac {\partial}{\partial z} (f V_y)[/tex]

Using the product rule

[tex]( f \frac {\partial{V_z}}{\partial {y}} + {V_z}\frac {\partial {f}}{\partial y})-(f \frac {\partial{V_y}}{\partial {z}} + {V_y}\frac {\partial {f}}{\partial z})[/tex]

Simplifying,

[tex]\frac {\partial}{\partial {y}} (f V_z +V_z f)-\frac {\partial}{\partial {z}} (f V_y+ V_y f)[/tex]

[tex]2f( \frac {\partial}{\partial {y}} V_z - \frac {\partial}{\partial {z}} V_y)[/tex]

[tex]2f \nabla \times \vec {v} \vert _x[/tex]

Where do i go from here? Or are my steps wrong?
 
Last edited:
kay,the code is \begin{array}{ccc} (3 columns)...

Okay.

Now solve your problem.

Daniel.
 
hmmm, I've tried it in the edited post above.
 
Well,use the Leibniz rule
[tex][\nabla\times (f\vec{V})]_{x} =[(\nabla f\times \vec{V})+f(\nabla\times\vec{V})]_{x} =...[/tex]

Daniel.
 
  • #10
lol, leibniz's rule did everything. But I've arrived at the solution already, thanks a lot.
 

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