Linear PDEs: A Simple Explanation

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Discussion Overview

The discussion revolves around the properties of linear partial differential equations (PDEs), specifically focusing on the nature of solutions to the equation u_{x}(x,t) = 1. Participants explore the implications of linearity and homogeneity in relation to the solutions of such equations.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions why the sum of two solutions to the PDE does not yield another solution, suggesting a misunderstanding of linearity.
  • Another participant clarifies that while the equation is linear, it is not homogeneous, which affects the summation of solutions.
  • A further reply explores the nature of the operator involved, indicating that the operator is linear in terms of its argument but maps to a nonzero function, complicating the linearity of the solution space.
  • One participant introduces the concept of homomorphisms and the kernel of the operator, explaining that the kernel contains solutions that map to zero, while the particular solutions map to a constant function, leading to a distinction between general and particular solutions.
  • Another participant suggests that the set of functions mapping to 1 can be expressed in terms of a particular solution plus elements from the kernel, emphasizing the structure of the solution space.

Areas of Agreement / Disagreement

Participants generally agree on the distinction between linear and homogeneous equations, but there remains some uncertainty regarding the implications of these properties on the solution space and the nature of the operator involved.

Contextual Notes

Limitations include the dependence on definitions of linearity and homogeneity, as well as unresolved aspects regarding the rewriting of the equation to achieve a mapping to zero.

malignant
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This isn't a homework problem so hopefully this section is fine.

I came across something that's bothering me while reviewing PDEs.
Take something like: u_{x}(x,t) = 1. which has the general solution: u(x,t) = c_{1}(t) + x. Wolfram says this is linear but if I take a different solution: v(x,t) = c_{2}(t) + x and add it to u it's not also a solution: u + v = c_{1}(t) + c_{2}(t) + 2x\\ (u + v)_{x} = 2 \neq 1

I must be missing something really simple here.
 
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It is a linear differential equation, but it is not homogeneous.
 
Orodruin said:
It is a linear differential equation, but it is not homogeneous.

Ahh, so the sum of solutions being a solution generally only applies to homogeneous equations?
 
yeah... you can think about it another way. Your operator is not linear. And so a sum of solutions is not necessarily a solution. Your solution is linear in the 'x' argument, but the operator is not linear on its 'argument' i.e. the function it is acting on.

edit: uh... wait, I did not say this properly... If you define your operator as ##\partial_x## then the operator is linear, but as you said, the operator is mapping to something nonzero (i.e. 1). And if you can somehow rewrite the equation so that it is mapping to zero, then the operator would no longer be a linear operator. But now that I think about it, maybe it is not possible to re-write this as a map going to 'zero'. So maybe ignore my post hehe sorry about that.
 
Last edited:
In terms of homomorphisms, let's call the linear operator ##\partial_x## a homomorphism from the vector space of functions to itself. (i.e. we have functions as the vectors and real numbers as the scalars of this vector space). Then the kernel of this homomorphism is simply the set of all functions such that the linear operator gives zero when it acts on them. And, generally the kernel of a homomorphism is a vector space itself. Therefore, the set of solutions are a vector space. Which is why adding two solutions gives another solution.

Instead, if we consider the set of functions such that the linear operator gives the constant function 1, what can we say about this set of functions? They all map to the same function. So this means that you can get one function by adding an element of the kernel to the other function. This is what we know more intuitively as particular solutions and homogeneous solutions. If you find one particular solution, then you can just add any solution of the homogeneous solution, to get the general solution.

So in your case, the kernel of the homomorphism is given by the set of all solutions to the equation ##\partial_x(f(x,t))=0## (which are of the form ##u(t)##). Also, one possible function which gets mapped to 1, is simply 'x'. Therefore, the set of all functions which get mapped to 1 are of the form ##u(t) + x##. I hope this explanation helped a bit.
 

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