Finding current density given B-field

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Homework Statement


Find the current density as a function of distance ##r## from the axis of a radially symmetrical parallel stream of electrons if the magnetic induction inside the stream varies as ##B=br^a##, where ##b## and ##a## are positive constants.


Homework Equations





The Attempt at a Solution


Honestly, I don't have any idea for this problem. I don't see any equations in my notes which relates the B-field and current density.

Any help is appreciated. Thanks!
 
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Pranav-Arora said:
I don't see any equations in my notes which relates the B-field and current density.
No, but I'm sure you have an equation for the field based on the current in a wire. Won't it just be a matter of integrating the density, viewed as many wire elements?
 
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haruspex said:
No, but I'm sure you have an equation for the field based on the current in a wire. Won't it just be a matter of integrating the density, viewed as many wire elements?

Ampere's circuital law?

[tex]\int \textbf{B}\cdot d\textbf{l} = \mu_o\int \textbf{J} \cdot d\textbf{S}[/tex]
What should I replace dl with? ##2\pi r##?
 
Pranav-Arora said:
Ampere's circuital law?

[tex]\int \textbf{B}\cdot d\textbf{l} = \mu_o\int \textbf{J} \cdot d\textbf{S}[/tex]
What should I replace dl with? ##2\pi r##?


Because of radial symmetry, the vector B is tangential to the circles around the axis and its magnitude depends only on the distance from the axis. dl=rdθ and yes, the line integral is B(2πr).

ehild
 
ehild said:
Because of radial symmetry, the vector B is tangential to the circles around the axis and its magnitude depends only on the distance from the axis. dl=rdθ and yes, the line integral is B(2πr).

ehild

That gives me
[tex]2\pi b r^{a+1}=\mu_o \int \textbf{J} \cdot d\textbf{S}[/tex]
Is ##dS=2\pi rdr##?

And how am I supposed to solve the above equation? :confused:
 
Pranav-Arora said:
That gives me
[tex]2\pi b r^{a+1}=\mu_o \int \textbf{J} \cdot d\textbf{S}[/tex]
Is ##dS=2\pi rdr##?

And how am I supposed to solve the above equation? :confused:

Plug in the expression for dS. The integral is valid for all r. You get an equation of form f(r)=0r∫g(r')dr'. How do you get g(r)?

ehild
 
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ehild said:
Plug in the expression for dS. The integral is valid for all r. You get an equation of form f(r)=0r∫g(r')dr'. How do you get g(r)?

ehild

Thank you ehild! :smile:

I get
[tex]br^{a+1}=\int_0^{r}\textbf{J}rdr[/tex]
Differentiating both the sides,
[tex]\Rightarrow (a+1)br^{a}=\textbf{J}r[/tex]
[tex]\Rightarrow \textbf{J}=(a+1)br^{a-1}[/tex]