Since \( f(x) = \frac{1}{2} [ g(x) + g(2 - x) ] \), we observe that \( f(x) \) is symmetric about \( x = 1 \), suggesting that the behavior around \( x = 1 \) is crucial.
Calculate \( f'(x) \):
\( f'(x) = \frac{1}{2} \left[ g'(x) + g'(2 - x) \right] \)
Given \( g'\left( \frac{1}{2} \right) = g'\left( \frac{3}{2} \right) \), we find:
\( f'\left( \frac{1}{2} \right) = \frac{1}{2} \left[ g'\left( \frac{1}{2} \right) + g'\left( \frac{3}{2} \right) \right] = 0 \)
and similarly,
\( f'\left( \frac{3}{2} \right) = 0 \)
Calculate \( f''(x) \):
\( f''(x) = \frac{1}{2} \left[ g''(x) - g''(2 - x) \right] \)
Since \( g \) is non-constant and twice differentiable, by the Intermediate Value Theorem, \( f''(x) = 0 \) must occur at least twice in \( (0, 2) \).
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).