Boas 4.12.18, 2nd Derivatives of Imp. Multivariable Integral

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SUMMARY

The discussion centers on the function u(x, y) = y/π ∫-∞∞ f(t) dt / ((x - t)² + y²) and its compliance with the Laplace equation, uxx + uyy = 0. Participants identified that the function does not satisfy the equation at y = 0 due to a discontinuity in the integrand. The Green's function of the Poisson equation in 2D is referenced, indicating that the function corresponds to a source term of the form f(x) δ'(y). The conversation emphasizes the importance of clarity in mathematical expressions and the application of Leibniz' Rule for differentiation under the integral sign.

PREREQUISITES
  • Understanding of the Laplace equation in two dimensions
  • Familiarity with Leibniz' Rule for differentiation under the integral sign
  • Knowledge of Green's functions in the context of partial differential equations
  • Proficiency in handling multivariable integrals and their derivatives
NEXT STEPS
  • Study the application of Green's functions in solving the Poisson equation
  • Learn about the properties and applications of the Laplace equation in physics
  • Explore differentiation techniques for integrals, specifically Leibniz' Rule
  • Investigate the implications of discontinuities in integrands when applying calculus
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Mathematicians, physicists, and engineering students who are working with multivariable calculus, particularly in the context of solving partial differential equations and understanding Green's functions.

mishima
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Homework Statement


Show that u(x, y) = y/π ∫-∞ f(t) dt / ((x - t)2+y2) satisfies uxx + uyy = 0.

Homework Equations


Leibniz' Rule

The Attempt at a Solution


I'm not even sure Leibniz' Rule can be applied here since there seems to be a discontinuity in the integrand when x=t and y=0. When I use it and take the second derivatives, I get terms that have no way of cancelling (for example the -2(x-t) and -2y terms). I also tried integration by parts first but it did not simplify things.
 
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You are correct. The function does not satisfy the Laplace equation in two dimensions at ##y = 0##. The Green's function of the Poisson equation in 2D is proportional to ##\ln(r^2/r_0^2)##. It is a matter of rather straight-forward computations to show that your function corresponds to a source term of the form ##f(x) \delta'(y)##, i.e.,
$$
u_{xx} + u_{yy} \propto f(x) \delta'(y).
$$
 
So my goal is to show the Laplace equation is satisfied for all other values of y?
 
For other values of ##y##, you should indeed get zero.
 
Are my first derivatives correct?

With (x-t)2+y2=g for compactness:

ux=-2xy/π∫f(t)dt/g2 + 2y/π∫t*f(t)dt/g2

uy=1/π∫f(t)dt/g - 2y2/π∫f(t)dt/g2
 
I suggest you remove the integral, ##\pi##, and ##f(t)## for readability. They will always be there. I also strongly recommend against splitting the ##(x-t)## into two terms in the first derivative wrt ##x##, but yes, they look correct.
 
$$ u_x = \frac {-2y(x-t)}{g^2}$$

$$ u_y = \frac {1}{g} - \frac {2y^2}{g^2} $$
 
Yes, that looks fine. Now the second derivatives.
 
$$u_{xx} = \frac {1}{g^2} - \frac {4(x-t)^2}{g^3}$$

$$u_{yy} = \frac {8y^3}{g^3} - \frac{6y}{g^2}$$

edit: oops I forgot the -2y in ##u_{xx}##
 
  • #10
You are missing the inner derivative of the first term in ##u_{xx}## and a factor 2 in the second term (one from the ##g^2## in the denominator and one from the inner derivative). You also have some sign errors.

Edit: Ok, what is missing is your factor ##-2y##. So what do you get when you do the sum?
 
  • #11
$$u_{xx} + u_{yy} = 8y \left( \frac {y^2-(x-t)^2}{g^3} - \frac {1}{g^2}\right)$$

Alright, I see it now. Thank you!
 
  • #12
Auxillary question, why is the factor of π included in u(x,y)? Is u a function that comes up in the sciences?
 
  • #13
The factor 1/pi is obviuosly irrelevant for whether or not you get zero. It is however an important overall factor in the definition of the Green’s function.
 
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  • #14
mishima said:

Homework Statement


Show that u(x, y) = y/π ∫-∞ f(t) dt / ((x - t)2+y2) satisfies uxx + uyy = 0.

Homework Equations


Leibniz' Rule

The Attempt at a Solution


I'm not even sure Leibniz' Rule can be applied here since there seems to be a discontinuity in the integrand when x=t and y=0. When I use it and take the second derivatives, I get terms that have no way of cancelling (for example the -2(x-t) and -2y terms). I also tried integration by parts first but it did not simplify things.
Your expression is ambiguous. I genuinely cannot tell if you mean
$$u(x,t) = \frac{y}{\pi} \int_{-\infty}^{\infty} \frac{f(t)}{(x-t)^2+y^2}\hspace{4ex}(1)$$
or
$$ u(x,t) = \frac{y}{\pi \int_{-\infty}^{\infty} \frac{f(t)}{(x-t)^2 + y^2} \, dt} \hspace{5ex}(2)$$
or, possibly, something else. Please use parentheses to make everything clear and unabmiguous (or, better still, use LaTeX to typeset your expressions, just as I have done in the above).
 

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