Bulgarian Drug Agency
Question
Asked 17th May, 2023
How to write δ(f(x,y)) in terms of δ function?
I know that δ(f(x))=∑δ(x−xi)/f′(xi). What will be the expression if "f" is a function of two variables, i.e. δ(f(x,y))=?
Most recent answer
K. Kassner You are right.
The method that I proposed may not work for all functions f(x,y), especially if they are continuous and do not have isolated zeros. In that case, one might try to separate the integrals or use a coordinate transformation as you suggested in your comment. For example, if we use polar coordinates $(r,\theta)$, then we have
$$\delta(f(r,\theta))=\frac{1}{r}\delta(r-r(\theta))$$
where $r(\theta)$ is the zero of f(r,$\theta$) as a function of r for a fixed $\theta$. This can be seen by using the Jacobian of the transformation and the property of the delta function.
All Answers (6)
Bulgarian Drug Agency
This is a challenging question. One possible way to write δ(f(x,y)) in terms of δ function is to use the following formula:
$$\delta(f(x,y)) = \sum_{i,j} \frac{\delta(x-x_i)\delta(y-y_j)}{|\nabla f(x_i,y_j)|}$$
where $(x_i,y_j)$ are the points where $f(x,y)=0$ and $\nabla f$ is the gradient of $f$. This formula is analogous to the one-variable case, but it requires that $f$ has isolated zeros and that $\nabla f$ does not vanish at those points.
Another possible way to write δ(f(x,y)) is to use the Fourier transform:
$$\delta(f(x,y)) = \frac{1}{(2\pi)^2}\int_{-\infty}^{\infty}\int_{-\infty}^{\infty} e^{-i(kx+ly)}\hat{\delta}(k,l) dk dl$$
where $\hat{\delta}(k,l)$ is the Fourier transform of $\delta(f(x,y))$, which can be computed by using the properties of the delta function and the Fourier transform.
To express δ(f(x, y)) in terms of the Dirac delta function, we can use the following representation:
δ(f(x, y)) = Σ [δ(x - x_i) δ(y - y_i)] / |∇f(x_i, y_i)|
Here's a breakdown of the components in this expression:
δ(x - x_i) and δ(y - y_i) are individual Dirac delta functions centered at specific points (x_i, y_i) that satisfy the equation f(x_i, y_i) = 0. These points are determined by the zeros of the function f(x, y).
|∇f(x_i, y_i)| represents the magnitude of the gradient of f at each of those zero points. ∇f denotes the gradient vector (∂f/∂x, ∂f/∂y), and |∇f| denotes its magnitude.
To evaluate δ(f(x, y)) at a particular point (x0, y0), you would substitute that point into the expression above, summing over all relevant zero points (x_i, y_i) that satisfy f(x_i, y_i) = 0. The resulting expression would then be the value of δ(f(x, y)) at (x0, y0).
Note that this representation assumes that the function f(x, y) is differentiable and has isolated zeros. If f(x, y) has multiple zeros that coincide at a single point, the expression needs to be modified accordingly
Kyushu University
To write δ(f(x, y)) in terms of the Dirac delta function, you can use the property of the delta function known as the sifting property. The sifting property states that if g(x) is a continuous function with a single root at x = a, then the integral of g(x) multiplied by the Dirac delta function δ(x - a) is equal to g(a).
Applying this property to the function f(x, y), you can express δ(f(x, y)) as follows:
δ(f(x, y)) = Σ[δ(x - xi, y - yi) / |∇f(xi, yi)|],
where the sum is taken over all points (xi, yi) where f(xi, yi) = 0, and ∇f(xi, yi) is the gradient of f evaluated at (xi, yi). The |∇f(xi, yi)| represents the magnitude of the gradient.
This expression accounts for the fact that the Dirac delta function is being evaluated at the points where f(x, y) is zero. The presence of the gradient magnitude in the denominator ensures that the Dirac delta function is appropriately weighted at each point to maintain the integral property.
It's important to note that the expression above assumes that f(x, y) is continuous and differentiable, and that the points (xi, yi) where f(xi, yi) = 0 are isolated. If f(x, y) has multiple roots or singularities, the expression may require modification to handle those cases appropriately.
Otto-von-Guericke-Universität Magdeburg
Lyudmil Antonov "but it requires that $f$ has isolated zeros and that $\nabla f$ does not vanish at those points"
Which seems difficult to achieve for continuous functions. In order for f to have isolated zeros, it cannot have both signs near the zero, otherwise there must be a curve through the zero separating the regions of positive and negative f(x,y). An example with an isolated zero would be f(x,y) = x2n+y2n, with n integer, which is purely positive around the isolated zero at (0,0). But then ∇f vanishes at the zero...
Applications of a delta function of two variables will typically involve continuous functions, not discontinuous ones, which would, moreover, not be differentiable at the discontinuity.
One way to deal with a situation as the one given in the question would be to separate the integral in an integral over x and y. Then y is a parameter for the x integral, and
δ(f(x,y))=∑iδ(x−xi(y))/|∂f(x,y)/∂x|x=xi(y),
where xi(y) are the zeros of f(x,y) as a function of x at the considered value of y.
If a simple separation of the integrals is not possible, then one might try to find a coordinate transformation (e.g. to polar coordinates), in which it is feasible. In any case, the delta function will remove only one integration, not all of them (assuming the expression is to be integrated over a surface).
Bulgarian Drug Agency
K. Kassner You are right.
The method that I proposed may not work for all functions f(x,y), especially if they are continuous and do not have isolated zeros. In that case, one might try to separate the integrals or use a coordinate transformation as you suggested in your comment. For example, if we use polar coordinates $(r,\theta)$, then we have
$$\delta(f(r,\theta))=\frac{1}{r}\delta(r-r(\theta))$$
where $r(\theta)$ is the zero of f(r,$\theta$) as a function of r for a fixed $\theta$. This can be seen by using the Jacobian of the transformation and the property of the delta function.
Similar questions and discussions
Were some scientists right in showing that the Lorentz Force brings to a paradox??
Stefano Quattrini
Several scientists pointed out a paradoxical consequence of the application of the Lorentz Force as an addendum to Maxwell's equations in the form given by Heaviside. There is at least one case where the momentum is not conserved...
From the script of 1911 Einstein and Laub to Coleman, Shockley, Furry, Boyer, Babson, Reynolds, Bjorkquist, Griffiths, and Mansuripur till 2012 it was pointed out such an issue.
See the link for details http://people.exeter.ac.uk/sh481/shockley-james.html
-----------
Einstein A and Laub J "Über die im elektromagnetischenFelde aus ruhende Körper ausgeubten pondermotorischeKräfte"
Ann. Phys. 26 541 (1911)
--------------
Coleman, S. and Van Vleck, J. H. "Origin of Hidden Momentum Forces on Magnets"
Phys. Rev. 171 1370 (1968)
------------
Shockley W "Hidden linear momentum related to the α,E term for a Dirac-electron wave packet in an electric field"
Phys. Rev. Lett. 20 3434 (1968)
-------------
Furry, W. H. "Examples of Momentum Distributions in the Electromagnetic Field and in Matter",
Am. J. Phys. 37 621 (1969)
--------------
Boyer, T. H. "Concerning hidden momentum",
Am. J. Phys. 76 190 (2008)
---------------
Babson, D., Reynolds, S. P., Bjorkquist, R. and Griffiths, D. J. "Hidden momentum, field momentum, and electromagnetic impulse",
Am. J. Phys. 77 826 (2009)
-----------------------------
Mansuripur M. Trouble with the Lorentz law of force: incompatibility with special relativity and momentum conservation.
Phys. Rev. Lett. 108 193901 (2012)
------------------------------
Apart from space-time, are there any other mathematical models of physical phenomena using a fourth dimension?
Robert Shour
I searched yesterday and could not find any references, apart from hypercubes etc, to mathematical modeling using 4 dimensions other than my articles on arXiv and RG. That may explain why the role of 4/3 scaling has been unnoticed by physics.
I think a fourth dimension does play a role in modeling:
3/4 metabolic scaling.
Peto’s paradox
Brain weight scaling
4/3 fractal envelope of Brownian motion.
Clausius 1860 article on gas molecular mean path lengths.
Waterston on the energy to maintain a levitating elastic plane in a gravitational field (Roy Soc 1892 publication of 1845 submission).
Dark energy.
Are there any others?
Several articles on RG discuss 4/3 scaling, which involves the 4th dimension, including:
Preprint Dark energy modeled by scaling
Preprint Flow as a fourth dimension
and several other RG articles back to .
Related Publications
We show that both $(\mathcal{H}(c_{0}),\tau_{\omega})$ and
$(\mathcal{H}_{b}(c_{0}),\tau_{b})$ have a monomial Schauder basis.