What is the meaning of the second equality in Griffiths equation 5.32?

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Homework Help Overview

This discussion revolves around a question from Griffiths' Electromagnetism textbook, specifically regarding the interpretation of a second equality in equation 5.32. The original poster expresses confusion about the meaning and formal definition of the integral involving a cross product in the context of the Biot-Savart Law.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • Participants explore the nature of the integral and its components, questioning how to interpret the path integral and the meaning of the differential elements involved. Some participants suggest breaking down the integral into its vector components and discuss the implications of the cross product in this context.

Discussion Status

The discussion is ongoing with various interpretations being explored. Some participants provide insights into the definitions of differentials and vector fields, while others seek clarification on specific mathematical expressions. There is no explicit consensus yet, but several productive lines of inquiry are being pursued.

Contextual Notes

Participants note the relevance of the Biot-Savart Law and the context of magnetostatics, where current is considered steady. There is also mention of different coordinate systems and their implications for the definitions being discussed.

ehrenfest
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Homework Statement


This question refers to Griffiths E and M book.

The first equality makes perfect sense to me. It is a standard path-integral along the wire FOR EACH COMPONENT OF THE INTEGRAND. It is defined just like this (for each component)

\int_C f\, ds = \int_a^b f(\mathbf{r}(t)) |\mathbf{r}'(t)|\, dt

I do not understand the second equality at all. What exactly does

\int \frac{d\mathbf{l'}\times \hat{\mathbf{r}}}{r^2}

mean?

I have never seen an integral like. What is the formal definition of that integral? So, you parametrize your path and then do what? I just don't understand??!

BTW: how do you get that the script r that Griffiths uses in latex?

Homework Equations


The Attempt at a Solution

 
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The expression in the integrand is part of the Biot-Savart Law, the part that shows the magnetic field is inverse-square and that it is always orthogonal to the direction of the current element Idl and also to the radial component of the distance from the current. Because of this double orthogonality, you need a cross product notation. The permeability and current are taken out of the integrand because in what Griffiths calls magnetostatics, current is steady. That was an experimentally determined "law" based on observational data.

Some introductory textbooks have examples of how to actually perform this integration; for example, you can use it to find the field from a wire segment, and then expand the wire to infinity and get Ampere's law for a long wire.
 
It's three path integrals in wrapped up in one vector package. Define the path l' and treat each of the x,y and z components as a separate path integral.
 
Could you just write out exactly what this means:

\int_{\gamma} d\mathbf{l} \times \mathbf{v}

where \gamma: I \to R^3 [/tex] is a rectifiable path and \mathbf{v} is a continuous vector field? The object above is a vector, so can you write out the x-coordinate for me please?
 
How would you do a cross product?

What is the definition of : d\mathbf{l} [/itex] ?
 
malawi_glenn said:
What is the definition of : d\mathbf{l} [/itex] ?
<br /> <br /> Thats what I want to know.
 
ehrenfest said:
Thats what I want to know.

If you introduce an explicit Cartesian basis, then d\mathbf{l} = dx \hat{\mathbf{x}} + dy \hat{\mathbf{y}} + dz \hat{\mathbf{z}}
 
and in general (3-dimensions)

d\mathbf{r} = h_1 du_1 \mathbf{e}_{u_1} + h_2 du_2 \mathbf{e}_{u_2} + h_3 du_3 \mathbf{e}_{u_3}

where:
h_i = \vert \partial \mathbf{r} / \partial u_i \vert

\mathbf{e}_{u_i} = \frac{\partial \mathbf{r}}{ \partial u_i} / h_i

I thought Griffiths had these defenitions?
 
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What malawi and genneth wrote is different.
 
  • #10
ehrenfest said:
What malawi and genneth wrote is different.


why? The thing i wrote is the general definition, it reduces to what genneth wrote if you have a cartesian coordinate system. I can give the d\matbf{r} in spherical and/or cylindrical coordinates as well if you want?

In cartesian coordinates, all h_i = 1

u_1 = x, u_2 = y, u_3 = z and \hat{\mathbf{x}} = \mathbf{e}_{u_1} is just different notations for the same things, just as i call it d\mathbf{r}}, gennet calls it d\mathbf{l}},

I mean it just follows from the chain rule and the definition of differentials ( I know you have differentials and infenitesimals from another thread you created some weeks ago) :


d\mathbf{r} = \frac{\partial \mathbf{r}}{ \partial u_i}du_i (using einstein summation)

So by just saying that we says different things and not even trying to give it substance or showing that you have at least tried what I and gennet posted to you, makes me sad. I think that was a quit ignorant posting of you.

You should be glad that me and genneth, who 'works' here for free, helps you by posting here and in the other thread that you create here.
 
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  • #11
Oops, I missed the part where you said "and in general (3-dimensions)" and the part where genneth said "If you introduce an explicit Cartesian basis", sorry.

Also, sorry malawi that you are not supplied with a salary. In fact you have even given money to PF ironically. :)
 
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