Track refraction without changing the source frequency
Refraction changes ray direction when light passes between media with different speeds, except at normal incidence where direction can remain unchanged. Refractive index is n=c/v, with c the vacuum speed and v the phase speed in the stipulated medium. A larger index means a lower speed, not a larger frequency supplied by the source.
Learning outcome: Compare indices 1.2 and 1.8 at the same 40° incident angle, then repeat at 0°. Retain angle, speed, frequency and wavelength; explain which quantities change and which do not.
Starting recap
Define normal angles and signed object/image distances. Distinguish actual ray intersections from backward extensions, and keep the focal/critical boundaries explicit rather than forcing a finite answer.
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With n₁=1.00, n₂=1.50 and θ₁=30°, sinθ₂=1/3, so θ₂≈19.47°. Speed becomes 2.00×10⁸ m/s. Frequency stays 5.00×10¹⁴ Hz and wavelength becomes 400 nm.
Open the experimentPredict
At normal incidence, can speed and wavelength change even though the ray does not bend?
Experiment
Compare indices 1.2 and 1.8 at the same 40° incident angle, then repeat at 0°. Retain angle, speed, frequency and wavelength; explain which quantities change and which do not.
Infer refracted direction while preserving frequency
Worked teaching model · synthetic values · Incident medium n1=1.00, second n2 selected. Transparent nondispersive media for stipulated vacuum wavelength 600 nm; c=3.00×10⁸ m/s. Interface horizontal, light travels from upper medium to lower. Partial reflection intensity is not calculated.
Reset keeps your prediction, captures and practice history.
Physical ray direction follows its listed first coordinate to last coordinate. Dashed lines are not extra propagating rays. Display scale changes between settings; within the diagram both axes use the same scale.
| Segment | Coordinates in listed direction | Type |
|---|---|---|
| Incoming ray | (-0.64279, 0.76604) → (0, 0) | Physical ray |
| Reflected direction (intensity not modeled) | (0, 0) → (0.64279, 0.76604) | Physical ray |
| Transmitted direction | (0, 0) → (0.42853, -0.90353) | Physical ray |
| Interface | (-1, 0) → (1, 0) | Extension / construction |
| Normal | (0, -1) → (0, 1) | Extension / construction |
| Quantity | Value | Unit |
|---|---|---|
| Incident index | 1 | ratio |
| Transmitted index | 1.5 | ratio |
| Incident speed | 300000000 | m/s |
| Second-medium speed | 200000000 | m/s |
| Transmitted ray angle | 25.374 | degrees |
| Frequency | 500000000000000 | Hz |
| Wavelength in second medium | 400 | nm |
Accessible plot coordinates
Light changes speed and wavelength across the interface while frequency stays fixed.
Angles are from the normal. Refracted direction comes from n1 sinθ1=n2 sinθ2. Drawn reflected and transmitted directions do not imply equal intensities. At normal incidence the speed can change with no bending. Total internal reflection requires travel from higher to lower index.
Light changes speed and wavelength across the interface while frequency stays fixed.
Angles are from the normal. Refracted direction comes from n1 sinθ1=n2 sinθ2. Drawn reflected and transmitted directions do not imply equal intensities. At normal incidence the speed can change with no bending. Total internal reflection requires travel from higher to lower index.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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Public practice checks a specific claim. It does not establish independent mastery.
Why is a change in wavelength not evidence that the stationary interface changed the source frequency?
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