The Clues in the Shadows
Imagine you are standing in front of a mysterious spherical mirror. You place a tall object, exactly 100 cm in height, on the principal axis.
The mirror casts an image that is 25 cm tall. But here is the most crucial piece of evidence: the image has the same orientation as the object.
In the realm of optics, an image that stands upright (same orientation) is always a virtual image. It is an optical illusion formed by the diverging rays of light, appearing to exist behind the mirror.
The Magnification Revelation
Let's quantify this observation. The magnification m of a mirror is the ratio of the image height hi​ to the object height ho​.
m=ho​hi​​=100+25​=+41​
The positive sign mathematically confirms that the image is erect. More importantly, the value 41​ is less than 1, which means the image is diminished (smaller than the object).
The Identity of the Mirror
Now, we must play detective. Which type of spherical mirror can produce an image that is both virtual and diminished?
A concave mirror can indeed form a virtual image, but only when you stand very close to it. However, that virtual image is always magnified (like a makeup mirror).
A convex mirror, on the other hand, always scatters light outwards. No matter where you place a real object, a convex mirror will always form a virtual, erect, and diminished image. Therefore, our mysterious mirror is undeniably convex!
The Mathematical Proof
Let's solidify our logical deduction with rigorous mathematics. We know the absolute focal length is 40 cm. For a convex mirror, the focus lies behind the mirror, so f=+40 cm.
Using the magnification formula in terms of focal length:
Substituting our known values:
Solving for the object distance u:
Now, let's find the exact location of the image using the standard magnification relation:
The positive sign of v is the final nail in the coffin. It proves that the image is formed 30 cm behind the mirror, on the opposite side of the object.
Thus, we can confidently conclude that the image is virtual and located on the opposite side of a convex mirror.