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SCIENCE · INVESTIGATE AND EXPLAIN

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.

Starting recap

Retain complex amplitude before intensity, definite-integral boundaries, normalization, calibration covariance and unused evidence.

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Try

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 experiment

Predict

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.

Reset keeps your prediction, captures and practice history.

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.

objectlenssensorAxial spacings are schematic; signed heights share one scale.
Original conditional optical ledger
QuantityValueUnit
Matrix A-1ratio
Matrix B-10cm
Matrix C-0.100000inverse cm
Matrix D-2ratio
Matrix determinant1ratio
Imaging-plane distance15cm
In-focus magnification-0.500000ratio
Sensor ray-height spread0.400000cm
Largest output angle approximation0.0500000radians
Local tangent relative discrepancy0.000834168ratio
  • 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.

Virtual original records only. No laser, intense-light source, instrument alignment, physical apparatus operation or completed practical competence is supplied.

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.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

1. Establish the optical mechanism

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.

For object distance a and sensor distance b, apply the matrices in travel order: M=P(b)L P(a). Multiplication gives A=1−b/f, B=a+b−ab/f, C=−1/f and D=1−a/f. The determinant is one in this same-index ray convention, a useful independent consistency check.

Final height is Ay+Bθ. Rays from one object point have different starting angles, so they meet at one image height only when B=0. Solving gives b=fa/(a−f) and magnification A=−b/a. A sensor placed elsewhere retains angle-dependent spread; selecting one ray does not demonstrate focusing.

The original packet uses f=10 cm, object height 0.1 cm and three angles −0.02,0,+0.02 rad. It reports a local tanθ/θ discrepancy at the largest predicted output angle to illustrate one small-angle approximation. That is not a complete aberration bound: finite thickness, aperture clipping, diffraction and actual lens design remain omitted.

2. Work the original evidence

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.

3. Predict and investigate

Which matrix entry must vanish for a common object point to image independently of the initial ray angle?

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.

Transfer the derivation to a changed case

At a=40 cm, find the paraxial image distance and magnification. Would b=10 cm be that image plane?

Retain your prediction, intermediate reasoning and assumptions before opening public feedback.

Compare a worked response

Image distance is 400/30=13.3333 cm and magnification −1/3. At b=10, B=40+10−40=10 cm, so it is not the image plane for this finite object.

Primary mechanism context. Checked 31 October 2026. Original prose, records and diagrams; no copied source exercises or physical light-source operation. Retain first reasoning and public-feedback exposure in the course evidence workspace when registered.

Apply

What does B=0 mean in the declared ray column convention?

Public practice checks a specific claim. It does not establish independent mastery.

At a=40 cm, find the paraxial image distance and magnification. Would b=10 cm be that image plane?

Continue

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