80 cm
70 cm
90 cm
60 cm
For S1, μ₂/v - μ₁/u = (μ₂ - μ₁)/R
Substituting the respective values we get,
1/v - 1.5/(-50) = (1 - 1.5)/10
or 1/v + 3/100 = -1/20
v = -50 cm
This acts as an image for S2 with distance from its aperture as d - 50 cm. For parallel rays to emerge from S2, the image must be at infinity. Therefore, for S2:
μ₂/v - μ₁/u = (μ₂ - μ₁)/R
1/∞ - 1.5/(d-50) = (1 - 1.5)/10
0 - 1.5/(d - 50) = -0.5/10
1.5/(d - 50) = 1/20
d - 50 = 30
d = 80 cm