Thin-lens equation
Relates signed focal length, object distance, and image distance for a thin lens.
Concept module
Trace principal rays through converging and diverging lenses, connect the signed thin-lens equation to the diagram, and watch image distance and magnification respond to the same object setup.
The simulation shows a thin lens at the center of the principal axis, an object arrow to the left, and an image arrow that moves according to the signed thin-lens equation. Depending on the setup, the image arrow appears on the far side as a real inverted image or on the object side as a virtual upright image. Optional overlays show the focal markers, the principal rays, and the distance-and-height guide used in magnification. The converging lens uses signed focal length 0.8 m. An object at 2.4 m with height 1 m forms a inverted, smaller real image at 1.2 m, with magnification -0.5.
Interactive lab
Keep the stage, graph, and immediate control feedback in one working view.
Lens Imaging
Drag the object arrow or use the controls. The ray diagram, signed distances, and response graphs stay on the same thin-lens model.
Lens state
Graphs
Switch graph views without breaking the live stage and time link.
Object to image map
Shows how the signed image distance responds when you move the object while keeping the same lens.
Controls
Adjust the physical parameters and watch the motion respond.
Controls the focal points and how sharply the rays bend.
Moves the object along the principal axis.
Changes the object size so the magnified image height can be compared directly.
Presets
Predict -> manipulate -> observe
Keep the active prompt next to the controls so each change has an immediate visible consequence.
Try this
Equation map
Select a symbol to highlight the matching control and the graph or overlay it most directly changes.
Sets how strongly the lens bends the rays. The sign comes from the lens-type toggle: converging uses positive f, diverging uses negative f.
Equations in play
Choose an equation to sync the active symbol, control highlight, and related graph mapping.
More tools
Detailed noticing prompts, guided overlays, and challenge tasks stay available without taking over the main bench.
What to notice
Use the live prompt to connect the signed equation, the rays, and the graph branch that the current setup lives on.
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Why it matters
Guided overlays
Focus one overlay at a time to see what it represents and what to notice in the live motion.
Overlay focus
Shows the focal points and twice-focal points on both sides of the lens.
What to notice
Why it matters
The focus markers anchor the standard lens-regime language directly on the stage.
Challenge mode
Use the real lens controls and graphs to hit image targets. The checks read the live signed distances and magnification instead of a separate puzzle state.
2 of 4 checks
Suggested start
The checklist updates from the live simulation state, active graph, overlays, inspect time, and compare setup.
Thin-lens equation
Relates signed focal length, object distance, and image distance for a thin lens.
Magnification
Gives the size ratio and the orientation sign of the image.
Sign rule
Positive image distance means the refracted rays actually meet and the image can land on a screen.
Progress
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Try this setup
Copy the live bench state and reopen this concept with the same controls, graph, overlays, and compare context.
Stable links
Short explanation
Thin-lens imaging works when many rays from one object point leave the lens in a pattern that either meets at one image point or appears to meet there when you extend the rays backward. The ray diagram and the thin-lens equation are two views of that same geometry.
This module keeps the setup compact on purpose. You change lens type, focal length, object distance, and object height, then the signed image distance, image orientation, and magnification update together on the stage and in the response graphs.
Key ideas
Live worked example
0.8 m
2.4 m
1. Start from the thin-lens relation
2. Rearrange for the signed image distance
3. Invert the result
Signed image distance
Common misconception
A diverging lens spreads light out, so it does not make an image at all.
A diverging lens still makes an image. The refracted rays separate, but their backward extensions meet at a virtual image on the object side.
That is why the image is upright, reduced, and cannot be projected onto a screen even though it is still a legitimate image point in the geometry.
Mini challenge
Prediction prompt
Check your reasoning
Quick test
Reasoning
Question 1 of 4
Choose one answer to reveal feedback, then test the idea in the live system if a guided example is available.
Accessible description
The simulation shows a thin lens at the center of the principal axis, an object arrow to the left, and an image arrow that moves according to the signed thin-lens equation. Depending on the setup, the image arrow appears on the far side as a real inverted image or on the object side as a virtual upright image.
Optional overlays show the focal markers, the principal rays, and the distance-and-height guide used in magnification.
Graph summary
The object-image graph plots signed image distance against object distance for the current lens family and focal length.
The magnification graph plots m against object distance, so the sign and magnitude of the image scaling are visible without leaving the ray diagram.
Read next
These suggestions come from the concept registry, so the reason label reflects either curated guidance or the fallback progression logic.
Use plane, concave, and convex mirrors to track equal-angle reflection, signed image distance, and magnification on the same live ray diagram.
Image two nearby point sources through one finite aperture and see why diffraction, wavelength, and aperture diameter limit how sharply an optical system can separate them.
Watch one light ray cross a boundary, connect refractive index to speed change, and see Snell's law set the refracted angle, bending direction, and critical-angle limit on the same live diagram.