mnb96
- 711
- 5
Hello,
I consider two functions f:R^2 \rightarrow R and g:R^2 \rightarrow R, and the two dimensional convolution (f \ast g)(\mathbf{x}) = \int_{\mathbb{R}^2}f(\mathbf{t})g(\mathbf{x-t})d^2\mathbf{t}
I proved using the Fourier transform and the convolution theorem that the convolution of two "rotated" versions of f and g is equivalent to simply taking the convolution (f*g) and rotating it.
However I have troubles proving these statement using only the definition of convolution. I will show my attempt. There must be a mistake somewhere.
I consider an isometry (rotation) \phi:R^2\rightarrow R^2 and the two rotated versions of the functions: f(\phi(\mathbf{x})) and g(\phi(\mathbf{x})).
The convolution would be: \int_{\mathbb{R}^2}f(\phi(\mathbf{t}))g(\mathbf{x}-\phi(\mathbf{t}))d^2\mathbf{t} By setting \mathbf{y}=\phi(\mathbf{t}) and observing that d^2y = d^2t we get: \int_{\mathbb{R}^2}f(\mathbf{y})g(\mathbf{x}-\mathbf{y})d^2\mathbf{y} which is not the expected result. Where is the mistake?
I consider two functions f:R^2 \rightarrow R and g:R^2 \rightarrow R, and the two dimensional convolution (f \ast g)(\mathbf{x}) = \int_{\mathbb{R}^2}f(\mathbf{t})g(\mathbf{x-t})d^2\mathbf{t}
I proved using the Fourier transform and the convolution theorem that the convolution of two "rotated" versions of f and g is equivalent to simply taking the convolution (f*g) and rotating it.
However I have troubles proving these statement using only the definition of convolution. I will show my attempt. There must be a mistake somewhere.
I consider an isometry (rotation) \phi:R^2\rightarrow R^2 and the two rotated versions of the functions: f(\phi(\mathbf{x})) and g(\phi(\mathbf{x})).
The convolution would be: \int_{\mathbb{R}^2}f(\phi(\mathbf{t}))g(\mathbf{x}-\phi(\mathbf{t}))d^2\mathbf{t} By setting \mathbf{y}=\phi(\mathbf{t}) and observing that d^2y = d^2t we get: \int_{\mathbb{R}^2}f(\mathbf{y})g(\mathbf{x}-\mathbf{y})d^2\mathbf{y} which is not the expected result. Where is the mistake?