Take the 2-minute tour ×
Physics Stack Exchange is a question and answer site for active researchers, academics and students of physics. It's 100% free, no registration required.

EDIT [for aptness of this question to this site, read 'real world applications' as 'applications in Physics']

The concept of function (of the form $f : \mathbb{R} \to \mathbb{R}$ ) has been used in various real world applications of Mathematics. In almost all of the applications the general consideration such as approximating a given function with another function is viewed through a lens of mean square error or one of several other such very similar metrics.

My question is concerning the use of functions which have singularities. I've heard from some Physicists that the use of such functions is just a matter of mathematical taste as such functions could be easily approximated with smooth functions and hence the choice of using such functions is just a matter of mathematical taste and it wouldn't make any conceptual difference. I tend not to agree with such an argument because it all depends on the lens of approximation that is being used. If we do not use the metrics like the ones mentioned above then it could be different. A function which contains singularities is fundamentally conceptually different from a smooth function which approximates it no matter how good the approximation is.

So my question is, are there any applications of Mathematics in which functions with singularities are used not just as a matter of mathematical taste but for conceptual reasons ?

share|improve this question

migrated from math.stackexchange.com Jul 9 '11 at 5:44

This question came from our site for people studying math at any level and professionals in related fields.

1  
Because this question is asking for a list of examples of applications, and there won't be a single right answer, I've made the question community wiki. –  Zev Chonoles Jul 7 '11 at 7:48
    
I'm not sure even physicists would agree with the fact that singularities can always be smoothed out; consider the singular behaviour of the metric describing black holes, for example. –  Gerben Jul 7 '11 at 12:52
    
@Gerben : well, of course not all types of singularities can be smoothed out, definitely, most of the functions that physicists need are the ones that are twice differentiable everywhere, but when it comes to singularities like for example a function not being smooth which means there are points where the function has singularities of the type of being only differentiable only say 8 times. These types of singularities are accepted by physicists that they can be approximated by smooth functions. I did not mention this in the question as I thought of keeping it in a general sense. –  Rajesh D Jul 7 '11 at 13:54
    
I agree with @Zev C: this should be a community wiki. –  qftme Jul 15 '11 at 16:25

6 Answers 6

One example from physics that springs to mind is the Operator Product Expansion (OPE) particularly used in conformal field theory and string theory. The singular part of the OPE is the most important, while the regular part rarely plays a significant role. Conceptually, the singular part (often called the contraction) measures the non-commutativity of the operators.

share|improve this answer
    
'non-commutativity of the operators' is not very convincing to be a concept of Physics, unless more explanation is possible. I don't know much about CFT, but singularities are commonly used in math involving complex analysis which doesn't necessarily mean it has physical meaning i guess. looking at the answers so far it is not going the way I thought but exactly going the way i didn't intend it to go. –  Rajesh D Jul 9 '11 at 16:19
2  
@Rajesh D: I have to run, so just a quick comment: 'Non-commutativity of the operators' has well-established physical consequences, such as e.g., Heisenberg uncertainty relations en.wikipedia.org/wiki/… –  Qmechanic Jul 9 '11 at 17:09
    
-1; I don't think you seem to have understood the spirit of the question.just as other answers. –  Rajesh D Jul 17 '11 at 7:08
    
I sincerely apologize for the inappropriateness of my earlier comment. I should have typed this message long back but due to some reasons i couldn't remember about it. I had read the wikipedia page and I did refer a book of conformal field theory and browse through some pages which show that singular part is mathematically more significant in an equation. I should admit that my level of mathematical knowledge seemed barely sufficient to even get an intuitive feel of such concepts. But after your comment which says that H's uncertainty relations follow from it.... –  Rajesh D Aug 1 '11 at 15:40
    
But I don't know even the physical significance of Heisenberg's uncertainty relations. I thought that they followed from the time frequency resolution issues of the quantum state (correct me if i didn't get the terminology right here) function (i mean $\psi$) and that the probabilistic nature of the position and momentum of a particle given by a state function is the basis of the Quantum mechanics and the uncertainity relation just follows from the limitation of the spectro temporal resolution of state function. Please correct me where ever i am wrong and clarify my basic doubts. –  Rajesh D Aug 1 '11 at 15:45

[I understand you are looking for more of a pure mathematical take on this, but there are many more examples of these sorts of approximations in applied mathematics (a couple I will document below). Which of course must have a pure mathematical basis as many are to do with the differentiability of the underlying functions.]

Yes there are functions in which singularities are approximated by piece-wise continuous functions. I will assume for the sake of argument that you are not limiting this discussion to relativistic-type "singularities" which are understood as a point at which a given mathematical object is not defined, but also to those of a point of an exceptional set which fail to be well-behaved in some particular way, such as differentiability. In the latter case there are many examples in computational mathematics and mathematical physics where the discontinuity or singularity can cause mathematical instability. An example of this to name one would be the modelling of a shock wave or "jump discontinuity" in computational fluid dynamics. A sudden step-change in any given variable can cause the numerical scheme to become unstable and "blow-up" in this instance the evolution equations are smoothed using artificial dissipation to avoid this behaviour.

In fact there are many examples of such modelling in computational relativistic astrophysics. Not only in the modelling of shock waves etc. but also in the modelling of flow moving across entities such as event horizons when modelling flows from compact objects.

I am sure there are many more instances but these are a few I have thought of.

I hope this is of some use.

share|improve this answer

I agree the asker's opinion, an equation has its own category for its solution, a unconcerned breaking point or singularity is deadly to ruin the meaning and sometime far away off the real solution.

share|improve this answer

To simplify the computations in N-body simulations it is used to do $\frac{1}{(d+\epsilon)^2}\:(\epsilon>0)$ instead of $\frac{1}{d^2}$ to avoid collisions. In my opinion the singularity is mainly due to the discretisation method. Other way to deal with the problem is the use of a much shorter time unit (adaptative) in the region where stars get closer. In the real world, AFAIK, there are no reports of star collisions, nor when galaxies are merging neither when they are heavily packed as it happens with clusters.

share|improve this answer

There are functions with singularities that arise all the time in physics. For example, an undamped (no friction) harmonic oscillator of mass $m$ driven by $F(t)=F_0\sin \omega t$ will have infinite amplitude at the resonance frequency, for the amplitude is given by $$ A(\omega)=\frac{F_0/m}{\omega^2-\omega_0^2}, $$ where $\omega_0=\sqrt{k/m}$ is the resonance frequency. Therefore, $\omega=\omega_0$ is a singularity of $A(\omega)$.

It's true that there are no undamped oscillators in nature, and the above equation is modified: $$ A(\omega)=\frac{F_0/m}{\sqrt{(\omega^2-\omega_0^2)^2+\left(\frac{b\omega}{m}\right)^2}}, $$ where $b$ is a constant that comes in with the friction term.

However, when, for example, mechanics build suspension systems for cars, they make sure that the typical frequency of oscillation of the system is far away from the resonance frequency, so that the car does not start oscillating violently when the driver goes over a bump.

Another example (this involves no idealization) comes from quantum field theory, and it is that physical masses of particles appear as poles of the Fourier-transformed two-point function of the field corresponding to the particle. So there is a function there that has a pole (singularity) when its variable becomes equal to the mass of the physical particle.

share|improve this answer

I can recall solving -1D differential equations in the 70's using the Galerkin method. If solutions that have singularities are present it is possible to incorporate the form of the singularity into one or more basis functions. Of course the weight function has to be choosen carefully, so that for instance all neccessary integrals are finite (usually the intgral of two basis functions times the weight function). As long as the positions and form of the singularities are known beforehand this seemed to work well.

share|improve this answer

Your Answer

 
discard

By posting your answer, you agree to the privacy policy and terms of service.

Not the answer you're looking for? Browse other questions tagged or ask your own question.