Correct option is C. $$w_0\left(1\mp \dfrac{2\omega v'}{g}\right)$$
When the ship is at rest: $$g_e=g-\omega^2R$$ ... (1)
When the ship is moving with velocity v' from west to east
$$\omega'=\omega_e+\omega_b$$
When the ship is moving east to west
$$\omega'=\omega_e-\omega_b$$
On combing the equations we can write:
$$\omega'=\omega_e\pm\omega_b$$
$$\Rightarrow \omega'=\omega\pm\dfrac{v'}{R}$$
g effective of the ship then becomes:
$$g_e'=g-R(\omega\pm\dfrac{v'}{R})^2$$
$$\Rightarrow g_e'=g-R(\omega^2\pm\dfrac{2\omega v'}{R}+\dfrac{v'^2}{R^2})$$
The last term is very small and can be neglected
$$\Rightarrow g_e'=g-R(\omega^2\pm\dfrac{2\omega v'}{R})$$
$$g_e'=g-R\omega^2\mp2\omega v'$$
From Eq 1:
$$g_e'=g_e\mp2\omega v'$$
$$g_e'=g_e(1\mp\dfrac{2\omega v'}{g_e})$$
multiplying boths sides by the mass m and using weight w=mg, we get,
$$\Rightarrow W'=W_o(1\mp\dfrac{2\omega v'}{g_e})$$