Step 1: The sound level in decibels is
\[\beta=10\log_{10}\!\left(\frac{I}{I_0}\right)\]
The change in level is
\[\Delta\beta=10\log_{10}\!\left(\frac{I_2}{I_1}\right)\]
Step 2: Here \(\Delta\beta=60-50=10\,\text{dB}\), so
\[10=10\log_{10}\!\left(\frac{I_2}{I_1}\right)\Rightarrow\log_{10}\!\left(\frac{I_2}{I_1}\right)=1\Rightarrow\frac{I_2}{I_1}=10\]
Step 3: Sound intensity is proportional to the square of the pressure amplitude:
\[I\propto p_0^{2}\quad\Rightarrow\quad\frac{p_{0,2}}{p_{0,1}}=\sqrt{\frac{I_2}{I_1}}\]
Step 4: Therefore
\[\frac{p_{0,2}}{p_{0,1}}=\sqrt{10}\]
\[\boxed{\sqrt{10}}\]