Answer:
[tex]h = 18.75 m[/tex]
Now when it will reach at point B then its normal force is just equal to ZERO
[tex]N_B = 0[/tex]
[tex]F_n = 1.72 \times 10^4[/tex]
Explanation:
Since we need to cross both the loops so least speed at the bottom must be
[tex]v = \sqrt{5 R g}[/tex]
also by energy conservation this is gained by initial potential energy
[tex]mgh = \frac{1}{2}mv^2[/tex]
[tex]v = \sqrt{2gh}[/tex]
so we will have
[tex]\sqrt{2gh} = \sqrt{5Rg}[/tex]
now we have
[tex]h = \frac{5R}{2}[/tex]
here we have
R = 7.5 m
so we have
[tex]h = \frac{5(7.5)}{2}[/tex]
[tex]h = 18.75 m[/tex]
Now when it will reach at point B then its normal force is just equal to ZERO
[tex]N_B = 0[/tex]
now when it reach point C then the speed will be
[tex]mgh - mg(2R_c) = \frac{1}{2]mv_c^2[/tex]
[tex]v_c^2 = 2g(h - 2R_c)[/tex]
[tex]v_c = 13.1 m/s[/tex]
now normal force at point C is given as
[tex]F_n = \frac{mv_c^2}{R_c} - mg[/tex]
[tex]F_n = \frac{700\times 13.1^2}{5} - (700 \times 9.8)[/tex]
[tex]F_n = 1.72 \times 10^4[/tex]