Right choice is (a) cl=\(\frac {4α}{\sqrt {M_∞^2-1}}\)
The best I can explain: Using linearlized theory, we can calculate the lift over a flat plate in supersonic flow. This is done by first calculating the the pressure over the upper and the lower surface.
cp,l=\(\frac {2α}{\sqrt {M_∞^2-1}}\)
cp,u=\(\frac {-2α}{M_∞^2-1}\)
The upper surface is inclined away from the free stream thus it has a negative value.
The normal and axial forces are computed as follows:
cn=\(\frac {1}{c} \int _0^c\) (cp,l-cp,u)dx=\(\frac {1}{c} \int _0^c \big ( \frac {2α}{\sqrt {M_∞^2-1}}-\frac {-2α}{\sqrt {M_∞^2-1}} \big ) \)dx
cn=\(\frac {4α}{\sqrt {M_∞^2-1}}\)
Similarly,
ca=\(\frac {1}{c} \int _{LE}^{TE}\)(cp,u-cp,l)dy=0
The value above is zero because for a thin plate of negligible thickness, dy=0.
Substituting the normal and axial forces in coefficient of lift formula:
cl=cncosα-casin∝=cn-ca∝
This is because the value of ∝ is very very small resulting in cosα~1,sinα~α.
cl=\(\frac {4α}{\sqrt {M_∞^2-1}}\)