(N/A) Given: Image distance $v = 100 \, cm$. Since the image is real and inverted, magnification $m = -2$.
Using the magnification formula $m = \frac{v}{u}$, we have $-2 = \frac{100}{u}$, which gives $u = -50 \, cm$.
Thus, the object should be placed at a distance of $50 \, cm$ in front of the lens.
Using the lens formula $\frac{1}{f} = \frac{1}{v} - \frac{1}{u}$, we get $\frac{1}{f} = \frac{1}{100} - \frac{1}{-50} = \frac{1+2}{100} = \frac{3}{100}$.
So, $f = \frac{100}{3} \, cm = \frac{1}{3} \, m$.
The power of the lens $P = \frac{1}{f(\text{in } meters)} = \frac{1}{1/3} = 3 \, D$.
$(b)$ The laws of refraction are:
$1$. The incident ray, the refracted ray, and the normal to the interface of two transparent media at the point of incidence all lie in the same plane.
$2$. Snell's Law: The ratio of the sine of the angle of incidence to the sine of the angle of refraction is a constant for the light of a given color and for the given pair of media, i.e., $\frac{\sin i}{\sin r} = \text{constant}$.