Simple integral, example or general solution correct?

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The forum discussion centers on the integration by parts technique applied to a multi-variable integral involving a density function, η(𝑥). The user initially attempts to integrate the expression ∫ d𝑘 𝑘ₓ f(𝑥,𝑘) and encounters contradictions in their results. Key insights reveal that the integration by parts was incorrectly applied, particularly regarding the treatment of surface terms and the need for proper limits of integration. The correct approach involves recognizing the role of the derivative of f with respect to 𝑘ₓ and ensuring the surface term is evaluated correctly.

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ExtravagantDreams
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This should be very simple, but I can find a simple example that violates my general conclusion. I clearly must be doing something wrong with my integration by parts. Any suggestions would be great.

Define a distribution such that the density;
\eta(\vec{x})=\int d\vec{k} f(\vec{x},\vec{k})
which is a function ONLY of x.

Now, let me arbitrarily calculate
\int d\vec{k} k_{x} f(\vec{x},\vec{k}) = \int dk_{x} k_{x} \int dk_{y} \int dk_{z} f(\vec{x},\vec{k})

I should be able to integrate over kx by parts;
k_{x} \int dk_{x} \int dk_{y} \int dk_{z} f(\vec{x},\vec{k}) - \int dk_{x} \frac{d k_{x}}{d k_{x}} \int dk_{x} \int dk_{y} \int dk_{z} f(\vec{x},\vec{k}) = k_{x} \int d\vec{k} f(\vec{x},\vec{k}) - \int dk_{x} \int d\vec{k} f(\vec{x},\vec{k})

Using the stipulation at the beginning this is simply;
k_{x} \eta(\vec{x}) - \int dk_{x} \eta(\vec{x})

Since, the density, eta, is only a function of x, this is zero.

There must be something wrong with this because I can come up with a simple example that contradicts this;

Let
f(\vec{x},\vec{k})=\eta(\vec{x})\delta (\vec{k}-\vec{k'})
It is easy to see that
\eta(\vec{x})=\int d\vec{k} f(\vec{x},\vec{k})

Now calculating the original quantity
\int d\vec{k} k_{x} f(\vec{x},\vec{k}) = \int dk_{x} k_{x} \eta(\vec{x})\delta (k_{x}-k'_{x}) = \eta(\vec{x}) k'_{x}

What gives? Where have I gone wrong?
 
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Your integration by parts looks incorrect. The surface term should not contain an integral over k_x, since that is the integration variable for which you are doing the integration by parts. Also, you should get something involving the derivative of f with respect to k_x, in the next term, and there should not be two integrals over k_x there.

Sometimes it is also good to write out the limits of the integration domains.

Torquil
 
Well, I'm taking u as k_x and v' as f in the standard notation
\int u v' = u v| - \int u' v
therefore I will not have a derivative of f.

Not sure what you mean by surface term. I do realize this is an integral over three variables and I should use the divergence theorem in general. But since u is a function of one variable only, it should be seperable. The k space over which the integral exsists also shouldn't matter, but I will check again.
 
You integration by parts is incorrect. To clear things up, let g(\mathbf{k}) = \int dk'_x~f(k_x',k_y,k_z), where the k_x integral is done from some intial value (say -infinity) to an arbitrary k_x, so that the result is still a function of \mathbf{k}. Now, let's do the integral by parts, supposing that the k integrals run from 0 to infinity.

\int dk_x k_x \int dk_y \int dk_z~f(\mathbf{k}) = \left. k_x \int dk_y \int dk_z g(\mathbf{k}) \right|^{k_x = \infty}_{k_x = -\infty} - \int dk_x \int dk_y \int dk_z~g(\mathbf{k}).

Assuming the surface term (the first term on the right hand side) is zero at +/- infinity, this gives

\int dk_x k_x \int dk_y \int dk_z~f(\mathbf{k}) = - \int dk_x \int dk_y \int dk_z~g(\mathbf{k}).
 
Last edited:
Yes of course. v is the indefinate integral of v' and not over the boundary of the initial region. I should have realize this before. Thanks!

Then, is there anything to be done without knowing the exact form of f(k,x)?
 

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