We assumed frictionless flow in solving the bump case, Prob. P10.65, for which $V_{2}=1.21 \mathrm{m} / \mathrm{s}$ and $y_{2}=0.826 \mathrm{m}$ over the crest when $h_{\max }=15 \mathrm{cm}, V_{1}=1 \mathrm{m} / \mathrm{s},$ and
$y_{1}=1 \mathrm{m} .$ However, if the bump is long and rough, friction may be important. Repeat Prob. P10.65 for the same bump shape, $h=0.5 h_{\max }[1-\cos (2 \pi x / L)],$ to compute
conditions $(a)$ at the crest and $(b)$ at the end of the bump, $x=L .$ Let $h_{\max }=15 \mathrm{cm}$ and $L=100 \mathrm{m},$ and assume a
clean-earth surface.