Answer:
![w_(out)=319.1(BTU)/(lbm)](https://img.qammunity.org/2021/formulas/engineering/college/yl75nudf904mtj1ls035jq9supcq6o10ti.png)
Step-by-step explanation:
Hello,
In this case, for the inlet stream, from the steam table, the specific enthalpy and entropy are:
![h_1=1456.0(BTU)/(lbm) \ \ \ s_1=1.6413(BTU)/(lbm*R)](https://img.qammunity.org/2021/formulas/engineering/college/74gbeiiwzgvkd1gq6cgo5r0ibc33tg7hdh.png)
Next, for the liquid-vapor mixture at the outlet stream we need to compute its quality by taking into account that since the turbine is adiabatic, the entropy remains the same:
![s_2=s_1](https://img.qammunity.org/2021/formulas/engineering/college/le6nf8sgbv6ms8os46x7daelt6m65tlczi.png)
Thus, the liquid and liquid-vapor entropies are included to compute the quality:
![x_2=(s_2-s_f)/(s_(fg))=(1.6313-0.39213)/(1.28448)=0.965](https://img.qammunity.org/2021/formulas/engineering/college/7pnj3d59kj3lu7dlfvrt8j7fm9hmui3p41.png)
Next, we compute the outlet enthalpy by considering the liquid and liquid-vapor enthalpies:
![h_2=h_f+x_2h_f_g=236.14+0.965*933.69=1136.9(BTU)/(lbm)](https://img.qammunity.org/2021/formulas/engineering/college/7q140iaw8oyxq4a6bc1hwkdkwu8iqk6cav.png)
Then, by using the first law of thermodynamics, the maximum specific work is computed via:
![h_1=w_(out)+h_2\\\\w_(out)=h_1-h_2=1456.0(BTU)/(lbm)-1136.9(BTU)/(lbm)\\\\w_(out)=319.1(BTU)/(lbm)](https://img.qammunity.org/2021/formulas/engineering/college/hsrlcs15g55a6r5cswq0vxq01jianxgcyr.png)
Best regards.