Analyzing the Setup
Imagine you are standing in Region I, looking towards Region II through a curved glass window. This window is a spherical refracting surface. The object is placed in Region I, and we need to find exactly where its image forms.
To do this, we must carefully apply the Cartesian sign convention. Since light travels from left to right, we take the right direction as positive.
The object is placed 40 cm to the left of the surface, so the object distance is u=−40 cm. The surface is concave towards Region I, meaning its center of curvature also lies to the left. Thus, the radius of curvature is R=−25 cm.
The Master Equation
The behavior of light refracting at a single spherical surface is governed by a beautiful relationship:
Here, μ1 is the refractive index of the medium where the incident light originates (Region I, so μ1=1.25), and μ2 is the refractive index of the medium the light enters (Region II, so μ2=1.4).
Executing the Calculation
Let's substitute our known values into the master equation:
v1.4−−401.25=−251.4−1.25
First, we simplify the right side of the equation. The difference in refractive indices is 1.4−1.25=0.15. Dividing this by −25 gives us −5003.
On the left side, the two negative signs cancel out, leaving us with +401.25, which simplifies to 321.
Now, we isolate the term containing our unknown image distance, v:
To subtract these fractions, we find a common denominator, which is 4000.
v1.4=−400024−4000125=−4000149
Final Conclusion
Finally, we solve for v:
v=−1491.4×4000=−1495600≈−37.58 cm
The negative sign is crucial here. It tells us that the image is formed on the same side as the object (Region I). This means the refracted rays diverge, and the image is virtual. The distance of this image from the surface is 37.58 cm.