The thermal efficiency of the Rankine cycle is given by:
\[
\eta = \frac{\text{Work output} - \text{Work input}}{\text{Heat input}}.
\]
The heat input is the total work output, which is the sum of the high pressure and low pressure turbine outputs:
\[
\text{Heat input} = 750 + 1500 = 2250 \, \text{kJ/kg}.
\]
The work input to the pump is:
\[
\text{Work input} = 20 \, \text{kJ/kg}.
\]
Thus, the thermal efficiency is:
\[
\eta = \frac{2250 - 20}{2250} = \frac{2230}{2250} \approx 0.989.
\]
The quality of the steam at the exit of the low pressure turbine is approximately:
\[
\boxed{92 \, \text{to} \, 96 \, %}.
\]