The gravitational deflection of light results from the effects of general relativity is an important calculation.
Now, I'm wondering, if I were using a first-order approximation of the Schwarzschild metric at the very beginning, namely
$$ds^2 = -\frac{1}{(1+\frac{r_s}{r})}c^2dt^2 + (1+\frac{r_s}{r})dr^2 + r^2d\theta^2 + r^2sin^2\theta d\phi^2.$$
Would that lead to the same gravitational deflection of light or would that lead to a different result?