Line charge density expressed via Dirac delta function

In summary, the problem involves finding the surface charge density, sigma(x,y), for a wire with finite length L and total charge Q evenly spread along the wire with a constant linear charge density, lambda=Q/L. The wire is shaped in the x-y plane with a well-behaved curve, y=f(x). The equations used are Q = Int(lambda dl) for the line charge density and Q = Int(sigma(x,y) dx dy) for the surface charge density. The proposed solution, sigma(x,y) = lambda * delta(y-f(x)), does not give the correct Q value and the error in reasoning is discussed.
  • #1
Heirot
151
0

Homework Statement



Let's say we have a wire of finite length L with total charge Q evenly spread along the wire so that lambda=Q/L, linear charge density, is constant. The wire is shaped in x-y plane in some well behaved curve y = f(x). Find the surface charge density sigma(x,y).

Homework Equations



Q = Int(lambda dl) = Int ( Sqrt(1+(dy/dx)^2) dx) for line charge density
Q = Int(sigma(x,y) dx dy) for surface charge density

The Attempt at a Solution



The most logic thing to do would be to write sigma(x,y) = lambda * delta(y-f(x)), where delta(x) is Dirac's delta function. Unfortunately, this doesn't give the right Q, because integration of the delta function over y only give 1 and not the required Sqrt(1+(dy/dx)^2).

Where's the error in reasoning?
 
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  • #2
But

[tex]
\begin{equation*}
\begin{split}
Q &= \lambda L \\
&= \lambda \int \sqrt{1 + \left( \frac{dy}{dx}\right)^2} dx.
\end{split}
\end{equation*}
[/tex]

Heuristically, the amount of charge on the wire between [itex]x[/itex] and [itex]x + dx[/itex] is

[tex]dQ = \lambda dL = \lambda \sqrt{1 + \left( \frac{dy}{dx}\right)^2} dx.[/tex]
 
Last edited:
  • #3
I agree. So, dQ = sigma(x,y) dx dy. What's sigma(x,y)?
 

Related to Line charge density expressed via Dirac delta function

1. What is line charge density expressed via Dirac delta function?

Line charge density expressed via Dirac delta function is a mathematical expression used to describe the distribution of electric charge along a line. It is often used in electromagnetism and electrostatics to model the charge distribution along a thin wire or filament.

2. How is line charge density expressed via Dirac delta function different from other methods of describing charge distribution?

Unlike other methods, such as continuous charge distribution or discrete point charges, line charge density expressed via Dirac delta function allows for an infinitely thin charge distribution along a line. This can be useful in simplifying calculations and modeling systems with uniform charge distributions.

3. How is the Dirac delta function related to line charge density?

The Dirac delta function is a mathematical function that is used to model an infinitely narrow peak with an area of 1. When applied to line charge density, it indicates that the charge is concentrated at a single point along the line, rather than being spread out over a finite distance.

4. Can line charge density expressed via Dirac delta function be negative?

Yes, line charge density expressed via Dirac delta function can be negative. This means that the charge distribution along the line is oriented in the opposite direction of a positive charge. It is important to note that the magnitude of the charge is still positive, but the direction is reversed.

5. How is line charge density expressed via Dirac delta function used in practical applications?

Line charge density expressed via Dirac delta function is used in a variety of practical applications, such as modeling the electric field around a thin wire, calculating the potential energy of a charged particle moving along a wire, and analyzing the behavior of electric circuits. It is a useful tool for simplifying complex systems and making calculations more manageable.

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