(N/A) Let $m$ be the mass of the Earth.
Let $\omega_p$ and $\omega_a$ be the angular velocities of the Earth around the Sun at perihelion and aphelion,respectively.
According to Kepler's second law,the areal velocity is constant,which implies $r_p^2 \omega_p = r_a^2 \omega_a$.
Given $r_p = a(1-e)$ and $r_a = a(1+e)$,we have $\frac{\omega_p}{\omega_a} = \left(\frac{1+e}{1-e}\right)^2$.
Substituting $e = 0.0167$,we get $\frac{\omega_p}{\omega_a} = \left(\frac{1.0167}{0.9833}\right)^2 \approx 1.0691$.
Let $\omega$ be the average angular velocity corresponding to the mean solar day. Then $\omega^2 = \omega_p \omega_a$.
Thus,$\frac{\omega_p}{\omega} = \frac{\omega}{\omega_a} = \sqrt{1.0691} \approx 1.034$.
In one day,the Earth rotates $360^\circ$ relative to the stars,plus the angle $\theta$ it moves in its orbit. The solar day is $T = \frac{360^\circ + \theta}{\omega_{spin}}$.
Since $\theta \propto \omega_{orbit}$,the variation in the solar day is $\Delta T \approx T_{mean} \times \frac{\Delta \omega}{\omega_{spin}}$.
Calculating the extremes,the variation is approximately $\pm 8 \text{ s}$.
This calculation shows that the variation due to orbital eccentricity is small and does not fully explain the observed variations in the length of the day,which are also significantly affected by the tilt of the Earth's axis (obliquity).