Myopia Corrected: How the Diverging Lens Actually Works
1 · Predict
A myopic eye's diverging corrective lens (f = −70 cm here) is meant to make distant objects appear to be at the eye's far point instead. Does this work the same way no matter how far away the actual object really is?
- Within the object distances this bench can actually reach, the virtual image distance still varies a lot as the true object distance changes — it hasn't yet settled near the far point.
- Yes — for any sufficiently distant object, the diverging lens forms a virtual image very close to its own focal point (near the far point), regardless of the exact true distance.
- The corrective lens doesn't change the effective image distance at all.
2 · Set Up
- Open the myopia-corrected preset and press Reset. The corrective diverging lens has f = −70 cm, matching this eye's far point.
- Enable the corrective lens's image-distance readout.
- Set the true object distance for each trial (all reasonably far) and record the virtual image distance formed by the corrective lens.
3 · Collect Data
| True object distance d_o (cm) | Corrective lens's image distance d_i (cm) |
|---|---|
| 30.00 | |
| 60.00 | |
| 100.00 |
Plot image distance d_i (y-axis) against object distance d_o (x-axis) for your three trials. Is d_i bending toward the lens's focal length (−70 cm, the eye's far point)? How close does it get over the range the bench allows?
4 · Analyze
- For one trial, compute d_i from 1/f = 1/d_o + 1/d_i using f = −70 cm. Compare to the table.
- Your table shows d_i still changing substantially even at the largest object distance this bench can reach (d_o = 100 cm, d_i only 58.8% of the way to f = −70 cm). Using 1/f = 1/d_o + 1/d_i, explain why d_i needs d_o in the many hundreds of cm before it gets truly close to f — this correction genuinely only becomes near-perfect for objects much farther away than this bench can place them, not for every 'distant' object.
5 · Extend
- This is the actual mechanism behind corrective lenses: they don't change what the eye's own lens does — they pre-process the light so the eye 'sees' the corrected image at a distance it CAN already focus on. Explain why this means corrective lenses work WITH the eye's own optics rather than replacing them.
- Compare this experiment's fixed f = −70 cm to the myopia experiment's corrective-power calculation for far point = 70 cm (P = −100/70 ≈ −1.43 D, so f = 1/P ≈ −70 cm). Confirm these are the same lens, described two different ways (focal length vs. diopters).
The Physics Behind This Experiment
How Corrective Lenses Redirect Light
A diverging corrective lens with f equal to (the negative of) the eye's far point images a TRULY distant object — many hundreds of cm away, well beyond what a tabletop bench can reach — at (or very near) that far point, exactly where the myopic eye CAN still focus. Closer than that, as this lab sheet's own trials show, the image still shifts noticeably with object distance.
Optics
- Converging Lens: Real Images Beyond 2f
- The Focal Point: Where Images Escape to Infinity
- A Lens as a Magnifying Glass
- A Diverging Lens: Always Virtual, Always Reduced
- A Concave Mirror: Real Images Like a Converging Lens
- A Convex Mirror: Always a Reduced Virtual Image
- The Plane Mirror: A Special, Invariant Case
- Apparent Depth: Why a Pool Looks Shallower Than It Is
- Total Internal Reflection: The Critical Angle
- A Two-Lens Relay: Chaining Images Together
- The Compound Microscope: Two Lenses for High Magnification
- A Photographic Enlarger: Two Lenses for a Real, Bigger Image