Just try substituting these into the definition
[tex]F[f(x,y)](u,v)=\int^{\infty}_{-\infty}\int^{\infty}_{-\infty}f(x,y)e^{-i(ux+vy)}dxdy[/tex]
f.e. let's do the first one:
f(x+6,y):
[tex]F[f(x+6,y)]=\int^{\infty}_{-\infty}\int^{\infty}_{-\infty}f(x+6,y)e^{-i(ux+vy)}dxdy[/tex]
I'm going to make the next change of variables:
[tex]x->\tilde{x}-6[/tex]
The boundaries of the integral remains unchanged, and so does the differential, but we get:
[tex]\int^{\infty}_{-\infty}\int^{\infty}_{-\infty}f(\tilde{x},y)e^{-i(u\tilde{x}-6u+vy)}d\tilde{x}dy[/tex]
Notice that [tex]e^{i6u}[/tex] is constant wrt to the integration, so we pull it out and what we have left of the integral is simply the Fourier transform of f(x,y) [because x* is just a dummy variable]:
[tex]e^{i6u}\int^{\infty}_{-\infty}\int^{\infty}_{-\infty}f(\tilde{x},y)e^{-i(u\tilde{x}+vy)}d\tilde{x}dy=e^{i6u}f(u,v)[/tex]
This technique of variable change is the standard technique to observe how shift & scale of the time-domain (the original function) affects the frequency-domain (its Fourier transform).