Derive an image plane by composing ray transformations
A paraxial ray state is the column (y,θ), where y is signed height and θ is a small signed angle. Free propagation through length l maps y to y+lθ and keeps θ, giving P(l)=[[1,l],[0,1]]. A thin lens of focal length f changes angle to θ−y/f, giving L=[[1,0],[−1/f,1]]. Units matter: the off-diagonal entries are length and inverse length.
Learning outcome: Propagate all three rays explicitly through object-to-lens, lens deflection and lens-to-sensor stages. Compare with matrix multiplication and then solve B=0 without claiming diffraction-free real imaging.
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At a=30 cm and b=20 cm, M=[[-1,−10],[-0.1,−2]] and determinant is 1. The true paraxial image plane is 15 cm with magnification −0.5. At the selected sensor the three rays span 0.4 cm rather than one image point.
Open the experimentPredict
Which matrix entry must vanish for a common object point to image independently of the initial ray angle?
Experiment
Propagate all three rays explicitly through object-to-lens, lens deflection and lens-to-sensor stages. Compare with matrix multiplication and then solve B=0 without claiming diffraction-free real imaging.
Compose propagation and a thin lens
Worked teaching model · synthetic values · Original paraxial ray column(y,θ), propagation P(l)=[[1,l],[0,1]], thin lens L=[[1,0],[-1/f,1]], f 10 cm. Object height 0.1 cm and input angles −0.02,0,+0.02 rad. Sensor matrix P(b)L P(a); same refractive index, no aperture clipping, diffraction or aberration.
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B=0 is the imaging condition: final height then stops depending on the initial ray angle.
Original paraxial ray column(y,θ), propagation P(l)=[[1,l],[0,1]], thin lens L=[[1,0],[-1/f,1]], f 10 cm. Object height 0.1 cm and input angles −0.02,0,+0.02 rad. Sensor matrix P(b)L P(a); same refractive index, no aperture clipping, diffraction or aberration.
| Quantity | Value | Unit |
|---|---|---|
| Matrix A | -1 | ratio |
| Matrix B | -10 | cm |
| Matrix C | -0.100000 | inverse cm |
| Matrix D | -2 | ratio |
| Matrix determinant | 1 | ratio |
| Imaging-plane distance | 15 | cm |
| In-focus magnification | -0.500000 | ratio |
| Sensor ray-height spread | 0.400000 | cm |
| Largest output angle approximation | 0.0500000 | radians |
| Local tangent relative discrepancy | 0.000834168 | ratio |
- Input angle -0.02 rad: Object height 0.1 cm; lens height -0.5 cm; sensor height 0.1 cm; output paraxial angle 0.03 rad.
- Input angle 0 rad: Object height 0.1 cm; lens height 0.1 cm; sensor height -0.1 cm; output paraxial angle -0.010000000000000002 rad.
- Input angle 0.02 rad: Object height 0.1 cm; lens height 0.7 cm; sensor height -0.30000000000000004 cm; output paraxial angle -0.05 rad.
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B=0 is the imaging condition: final height then stops depending on the initial ray angle.
Original paraxial ray column(y,θ), propagation P(l)=[[1,l],[0,1]], thin lens L=[[1,0],[-1/f,1]], f 10 cm. Object height 0.1 cm and input angles −0.02,0,+0.02 rad. Sensor matrix P(b)L P(a); same refractive index, no aperture clipping, diffraction or aberration.
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At a=40 cm, find the paraxial image distance and magnification. Would b=10 cm be that image plane?
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