Fix a time TT, put τ=T−t>0\tau=T-t>0, and choose real exponents a,b1,…,bda,b_1,\ldots,b_d. Similarity variables for a field u(t,x)u(t,x) are

yi=xiτ−bi,s=−log⁡τ,U(s,y)=τau(T−τ,Dτy),y_i=x_i\tau^{-b_i},\qquad s=-\log\tau,\qquad U(s,y)=\tau^a u(T-\tau,D_\tau y),

where DτD_\tau is the corresponding . The field need not be invariant under this change of variables.

Derivative formulas

The for u=τ−aU(s,y)u=\tau^{-a}U(s,y) gives

∂tu=τ−a−1(aU+∂sU+∑ibiyi∂yiU),∂xiu=τ−a−bi∂yiU.\partial_tu=\tau^{-a-1}\left(aU+\partial_sU+\sum_i b_i y_i\partial_{y_i}U\right), \qquad \partial_{x_i}u=\tau^{-a-b_i}\partial_{y_i}U.

These formulas describe the coordinate change for any exponents. Whether they make a particular PDE autonomous requires substituting into that equation.