Setting the Stage
The Moving Object
Imagine you are standing in a lab, observing a convex lens. Far away, at a distance of 20 m to the left, there is an object. The lens has a focal length of 0.3 m. Suddenly, the object starts moving away from the lens at a steady speed of 5 m/s.
Our mission is to find out exactly how the image reacts to this movement. How fast does it move? And in which direction? To solve this, we need to bridge the gap between optics and kinematics.
The Master Equation
Lens Formula in Motion
The fundamental relationship that ties the object distance u, the image distance v, and the focal length f together is the classic lens formula:
But we aren't just looking for static positions; we are dealing with motion! Velocity is simply the rate of change of position with respect to time. So, let's differentiate our master equation with respect to time t. Remember, the focal length f of a solid glass lens doesn't change, so its derivative is zero.
Rearranging this gives us a beautiful relationship between the image velocity vi and the object velocity vo:
This tells us that the image velocity is simply the object velocity scaled by the square of the transverse magnification m=uv.
The Magnification Shortcut
We need the ratio uv. We could calculate v first using the lens formula, but there is a more elegant shortcut. By manipulating the lens formula, we can express the magnification directly in terms of the knowns, u and f:
Inverting this and dividing by u gives:
This shortcut is a lifesaver in exams, saving precious time and reducing the chance of calculation errors!
Crunching the Numbers
Now, let's plug in our values. We must be careful with our sign convention. The object is on the left, so u=−20 m. The focal length of a convex lens is positive, so f=+0.3 m. The object speed is vo=5 m/s.
To make the calculation smoother, let's multiply the numerator and denominator by 10:
Squaring the fraction and multiplying by 5:
The Directional Dance
We have the speed, but what about the direction? Let's look back at our velocity equation:
Notice that the magnification m is squared. This means that m2 is always strictly positive. Consequently, the image velocity vi will always have the exact same sign as the object velocity vo.
In physical terms, the image always moves in the same direction as the object.
Our object is moving away from the lens, which means it is moving to the left. Therefore, the image must also move to the left. Since the real image is formed on the right side of the lens, moving to the left means it is moving towards the lens.
And there we have it! The image moves at 1.16×10−3 m/s towards the lens.