A momentum coefficient, $\beta,$ is defined by $$\int_{A} u \rho u d A=\beta \int_{A} V \rho u d A=\beta \dot{m} V$$ Evaluate $\beta$ for a laminar velocity profile, Eq. 8.14 , and for a "power-law" turbulent velocity profile, Eq. $8.22 .$ Plot $\beta$ as a function of $n$ for turbulent power-law profiles over the range $6 \leq n \leq 10$ and compare with the case of fully developed laminar pipe flow.