Proof of the Change of Variables Formula
We sketch the proof of the change of variables theorem, showing why the Jacobian determinant appears as the correction factor when transforming multiple integrals.
Theorem: If is a diffeomorphism between bounded open sets in , then .
Step 1: The linear case.
For a linear transformation with an invertible matrix, we show for any measurable set .
First consider elementary row operations:
- Scaling row by : multiplies volume by , and by
- Adding a multiple of one row to another: preserves volume (shearing), and is unchanged
- Swapping rows: preserves volume, changes sign of
Since any invertible matrix is a product of elementary matrices, follows by multiplicativity.
For a linear : follows from the volume scaling and the substitution in Riemann sums.
Step 2: Infinitesimal linearization.
For a general diffeomorphism , the key idea is that is approximately linear near each point. At :
A small box near with volume is mapped approximately to a parallelepiped with volume .
Step 3: Riemann sum argument.
Partition into small boxes with volumes and sample points . The Riemann sum for the right side is:
The images approximately partition , and . So the above sum approximates: which is a Riemann sum for with the partition .
Step 4: Making this rigorous.
The rigorous proof uses the fact that is a diffeomorphism to control the error in the linear approximation uniformly on compact subsets. Specifically, for any and sufficiently fine partition:
This follows from the uniform continuity of on compact sets. Summing over all boxes and taking the limit as the partition becomes finer gives the change of variables formula.
Alternatively, one can prove the result first for maps using the inverse function theorem and a partition-of-unity argument, then extend to by approximation.
In the language of differential forms, the change of variables formula is simply the statement that integration of an -form is invariant under pullback: . The Jacobian determinant appears automatically from the pullback of . This elegant formulation generalizes immediately to integration on manifolds.