I think that in general, as you move away from a sound it gets softer due to the dissipation of energy. However, I can see possibilities using exotic configurations of air density where the sound does get louder. For example, imagine that the air density increases while retaining the same bulk modulus. Then, as you move away from the source, the sound velocity will drop, allowing a buildup of sound pressure, just like in a sonic boom.
Another, more subjective possiblity, is that the sound experiences nonlinear effects such as frequency-dependent modulation and disperson. In that case, a powerful sound source emmitting sound above your hearing threshold would be inaudible up close, but due to nonlinear effects, more of that high energy sound is modulated downwards to audbile frequencies.
From OPs Comment
If your sources (A and B) have amplitudes $a,b$ at $r_A=r_b=1$ then assuming we move a distance $\delta$ from both A and B simultaneously we have the formulas:
$I_A(\delta)=\frac{a}{(r_A+\delta)^2},I_B(\delta)=\frac{b}{(r_B+\delta)^2}$ assuming the inverse square energy dissipation. What we want to know is how the intensities change as we move away from both sources, if $r_A>r_B,\frac{a}{r_A^2}>\frac{b}{r_B^2}$. One way to look at this is the ratio of the two intensities as you move away:
$\frac{I_A(\delta)}{I_B(\delta)} = \frac{a(r_B+\delta)^2}{b(r_A+\delta)^2}=\frac{a}{b}(\frac{r_B+\delta}{r_A+\delta})^2, \\ \lim\limits_{\delta\rightarrow \infty}\frac{a}{b}(\frac{r_B+\delta}{r_A+\delta})^2 = \frac{a}{b}$
Therefore, if you precieve A as louder than B, then moving away from both will never let B be louder than A, let alone let the sound overall get louder.
Anyway, just a couple out there thoughts.