PrayogSetu • Optical Refraction & Total Internal Reflection Simulator
Theoretical Curve Current Angle Critical Angle
| Trial | Medium 1 | n₁ | Medium 2 | n₂ | Incident Angle (θ₁) | Refracted Angle (θ₂) | Critical Angle (θc) | Result / Phenomenon |
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\[ n_1 \sin(\theta_1) = n_2 \sin(\theta_2) \]
Where \(n_1\) and \(n_2\) are the dimensionless refractive indices of Medium 1 and Medium 2, \(\theta_1\) is the angle of incidence, and \(\theta_2\) is the angle of refraction measured relative to the normal line.
The refractive index \(n\) of an optical medium is defined as the ratio of light speed in vacuum (\(c \approx 3.00 \times 10^8 \text{ m/s}\)) to light speed in the medium (\(v\)):
\[ n = \frac{c}{v} \implies v = \frac{c}{n} \]
When light crosses a boundary into an optically denser medium (\(n_2 > n_1\)), its phase velocity decreases, causing the wavefronts to tilt and bend toward the normal.
When light travels from an optically denser medium into a rarer medium (\(n_1 > n_2\)), the refracted ray bends away from the normal (\(\theta_2 > \theta_1\)). The incident angle at which \(\theta_2 = 90^\circ\) is the Critical Angle (\(\theta_c\)):
\[ \sin(\theta_c) = \frac{n_2}{n_1} \implies \theta_c = \arcsin\left(\frac{n_2}{n_1}\right) \]
For incident angles greater than \(\theta_c\) (\(\theta_1 > \theta_c\)), no light passes into Medium 2. All light is entirely reflected back into Medium 1, a phenomenon known as Total Internal Reflection (TIR).