Evaluate ∇ x \overline{F}: "Curl of Vector F

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Homework Help Overview

The discussion revolves around evaluating the curl of a vector field defined as ∇ x \overline{F}, where \overline{F}(\overline{r}) = \overline{r}lnr. The position vector \overline{r} is expressed in Cartesian coordinates (x, y, z), and participants are exploring the implications of using different coordinate systems for this evaluation.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants are attempting to differentiate the components of the vector field to compute the curl, but there is uncertainty about the correct approach, particularly regarding the use of Cartesian versus spherical coordinates.
  • Some participants question the representation of the vector field in spherical coordinates and whether it simplifies the calculation of the curl.
  • There is confusion about the meaning of variables V and A in the context of the vector field and how to derive the unit vector necessary for calculations.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem. Some guidance has been offered regarding the use of spherical coordinates, but there is still uncertainty about the definitions and representations of the vector components.

Contextual Notes

Participants are navigating the complexities of coordinate transformations and the implications for calculating the curl of the vector field. There is a lack of consensus on the best approach, and some foundational concepts are being clarified.

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Homework Statement



Evaluate ∇ x \overline{F}, with \overline{F}(\overline{r}) = \overline{r}lnr, where \overline{r} = (x; y; z) is the position vector and r is the modulus of the position vector.

Homework Equations



The curl of a vector

The Attempt at a Solution



I recognise I am evaluating the curl of the Vector F, however when taking the derivatives of the x, y and z components respectively. I'm not sure if it should be as follows. (showing the first bit of the problem)

(∂F(z)/∂y - ∂F(y)/∂Z), ...

which becomes

(∂\overline{r}(z)lnr/∂y) - (∂\overline{r}(y)lnr/∂Z),

Im not sure if this is right and if I need to include the modulus of the vector r when differentiating \overline{r}lnr with respect to y or z.
 
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The way you did it is only applicable when the vector field is in Cartesian coordinates.But your vector field is in spherical coordinates and so its curl should be evaluated using the following formula:
f5c4b982600895f128fcb4c54e68a785.png
 
Im sorry, how is it in spherical coordinates? my vector is given with a position vector in (x,y,z), isn't that Cartesian?
 
Since the curl is a vector operator you can calculate in any coordinates you like. Here it's easier to use spherical coordinates then Cartesian ones, because in spherical coordinates your vector field (it's a curl of a vector field not simply a vector!) reads
\vec{V}(\vec{r})=r \hat{r} \ln r=A_r(r) \hat{r}.
You have to evaluate less derivatives than in Cartesian coordinates, but of course, you'll get the same result at the end.
 
I see. But I'm a little confused what V and A represent? I acknowledge you have used the unit vector multiplied by the magnitude of the vector r, as this is the same as the vector itself; but how am I suppose to obtain a value for the unit vector so I can use it?
 
K.QMUL said:
I see. But I'm a little confused what V and A represent? I acknowledge you have used the unit vector multiplied by the magnitude of the vector r, as this is the same as the vector itself; but how am I suppose to obtain a value for the unit vector so I can use it?

<br /> \hat r = \frac{1}{\sqrt{x^2 + y^2 + z^2}}(x \hat i + y \hat j + z \hat k)<br />
 
Thanks, but what do V and A represent?
 
vanhees71 said:
Since the curl is a vector operator you can calculate in any coordinates you like. Here it's easier to use spherical coordinates then Cartesian ones, because in spherical coordinates your vector field (it's a curl of a vector field not simply a vector!) reads
\vec{V}(\vec{r})=r \hat{r} \ln r=A_r(r) \hat{r}.
You have to evaluate less derivatives than in Cartesian coordinates, but of course, you'll get the same result at the end.

And in the above, doesn't the r\hat{r} just become (x\hat{i}+y\hat{j}+z\hat{k})
 
I should have written V_r, and it's the radial component of the vector field. Again: It's of course the very same field in spherical coordinates as you've written in Cartesian coordinates. It's really easier to use spherical coordinates here.
 
  • #10
K.QMUL said:
I see. But I'm a little confused what V and A represent? I acknowledge you have used the unit vector multiplied by the magnitude of the vector r, as this is the same as the vector itself; but how am I suppose to obtain a value for the unit vector so I can use it?

##\vec{V}## is what you called ##\vec{F}##. In Cartesian coordinates, you have ##\vec{F} = A_x \hat{x} + A_y \hat{y} + A_z \hat{z}## where the A's are functions of x, y, and z. Similarly, in spherical coordinates, you have ##\vec{F} = A_r \hat{r} + A_\theta \hat{\theta} + A_\phi \hat{\phi}## where the A's are functions of r, ##\theta##, and ##\phi##.
 

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