To solve this problem, we use the lens-maker's formula suitable for spherical surfaces:
\[ \frac{n_2}{v} - \frac{n_1}{u} = \frac{n_2-n_1}{R} \]
where \( n_1 = 1 \) (refractive index of air), \( n_2 = 1.5 \) (refractive index of glass), \( R = 10 \) cm (radius of curvature), \( u = -50 \) cm (distance of the light source from the surface, negative because it is in the opposite direction to the incident light), and \( v \) is the distance of the image from the surface.
Substitute the known values into the formula:
\[ \frac{1.5}{v} - \frac{1}{-50} = \frac{1.5 - 1}{10} \]
Solving this equation:
\[ \frac{1.5}{v} + \frac{1}{50} = \frac{0.5}{10} \]
\[ \frac{1.5}{v} + \frac{1}{50} = 0.05 \]
\[ \frac{1.5}{v} = 0.05 - \frac{1}{50} \]
\[ \frac{1.5}{v} = 0.05 - 0.02 \]
\[ \frac{1.5}{v} = 0.03 \]
\[ v = \frac{1.5}{0.03} \]
\[ v = 50 \] cm
Thus, the image is formed 50 cm inside the glass.