Dirac delta function in 2d polar coordinates

  • #1
Trollfaz
137
14
In 3 d spherical coordinates we know that
$$\triangledown \cdot \frac{\hat{\textbf{r}}}{r^2}=4π\delta^3(\textbf{r})$$
Integration over all## R^3## is 4π
So when we remove the third dimensions and enter 2d polar coordinates then
$$\triangledown \cdot \frac{\hat{\textbf{r}}}{r}=2π\delta^2(\textbf{r})$$
So the integral over ##R^2## is 2π?
 
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  • #2
First of all, note that your expressions are not written in any particular coordinates (apart from the interpretation of ##r## as a coordinate function and ##\hat{\boldsymbol r}## as the corresponding unit vector. In particular, the delta functions are not the product of the coordinate delta functions.

Apart from that: Yes. You can easily check the result by use of the divergence theorem and integration over a sphere/circle. In fact, that is one way to find the constant factors in front.
 
  • #3
I'm quoting the first expression from Introductions to Electrodynamics (David J. Griffiths) Section 1.5.3, Eqn 1.99
$$\triangle \cdot \frac{\hat{r}}{r^2}=4π\delta^3(r)$$
 
  • #4
Trollfaz said:
I'm quoting the first expression from Introductions to Electrodynamics (David J. Griffiths) Section 1.5.3, Eqn 1.99
$$\triangle \cdot \frac{\hat{r}}{r^2}=4π\delta^3(r)$$
You are missing the point (and hopefully misquoting Griffiths as the expression as written here makes no sense). The expression in your OP was correct. My comment was that it was not really something dependent on using spherical coordinates.
 
  • #5
right, integral in ##R^3-B_\epsilon(0)##, and use divergence thm

if your are curious about the equation everypoint (specially point 0), that is Dirac delta, try to understand it as a functional like ##<\delta, \varphi>##, that is ## \int \limits_{R^3} \delta \varphi ##
 

1. What is the Dirac delta function in 2D polar coordinates?

The Dirac delta function in 2D polar coordinates is a mathematical function used to model an infinitely small and infinitely high spike at a certain point in a two-dimensional space defined by polar coordinates (r, θ). In Cartesian coordinates, the Dirac delta function δ(x, y) at the origin is represented in polar coordinates as δ(r, θ), where it is typically expressed as δ(r) multiplied by a factor of 1/(2πr) to account for the polar coordinate system's radial symmetry and area element transformation.

2. How do you express the Dirac delta function in 2D polar coordinates?

In 2D polar coordinates, the Dirac delta function centered at the origin can be expressed as δ(r)/(2πr). This expression takes into account the area element in polar coordinates, which is r dr dθ. The δ(r) function represents the delta function with respect to the radial coordinate r, which spikes at r = 0. The division by 2πr normalizes the function over the angle θ, ensuring that the integral over the entire plane still yields 1.

3. How is the Dirac delta function used in 2D polar coordinates for physical applications?

In physical applications, the Dirac delta function in 2D polar coordinates is often used to represent point sources or sinks of physical quantities such as mass, charge, or intensity, located at a specific point in a radial system. For example, in electromagnetism, it can model a point charge, and in fluid dynamics, it might represent a point vortex. Its utility in solving differential equations in polar coordinates, where sources or initial conditions are localized at a point, is significant.

4. What is the integral of the Dirac delta function in 2D polar coordinates over the entire plane?

The integral of the Dirac delta function δ(r)/(2πr) over the entire plane in polar coordinates is 1. This is calculated by integrating over r from 0 to infinity and θ from 0 to 2π. The integral with respect to θ trivially gives 2π, and the integral of δ(r) with respect to r from 0 to infinity gives 1, thus confirming the normalization condition that the total integral of the delta function over the space it is defined must be 1.

5. How does the Dirac delta function behave at the origin and elsewhere in 2D polar coordinates?

In 2D polar coordinates, the Dirac delta function δ(r)/(2πr) is zero everywhere except at the origin (r = 0). At the origin, it is undefined but is considered to have an infinitely high spike, such that the integral in a small region around the origin yields a finite value of 1. This characteristic allows it to "select" the value at the origin in an integral involving a product with another function, effectively evaluating the function at the origin.

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