0.666667
1
flag
0.729728
rad
41.8103
deg
48.1897
deg
0.666667
1
flag
0.729728
rad
41.8103
deg
48.1897
deg
The Critical Angle Calculator determines the minimum angle of incidence at which total internal reflection (TIR) occurs when light travels from a denser optical medium into a less dense one. Total internal reflection is one of the most important phenomena in geometric optics, underpinning the operation of optical fibers, prisms, binoculars, and diamond cutting.
When a light ray passes from a medium with a higher refractive index (n₁) to one with a lower refractive index (n₂), it bends away from the normal. As the angle of incidence increases, the refracted ray bends further until it travels along the interface at exactly 90° to the normal. The angle of incidence at which this occurs is the critical angle θc. For any angle greater than θc, all light is reflected back into the denser medium—no refraction occurs.
The critical angle is derived directly from Snell’s law. Setting the refraction angle to 90°, we obtain $$\theta_c = \arcsin\!\left(\frac{n_2}{n_1}\right)$$ where n₁ is the refractive index of the incident medium and n₂ is that of the less dense medium. The critical angle exists only when n₁ > n₂; if the light enters a denser medium, total internal reflection cannot occur.
Optical fibers exploit TIR to transmit light over kilometers with minimal loss. The core of a fiber has a higher refractive index than the surrounding cladding, so light launched at angles exceeding the critical angle bounces along the fiber indefinitely. Similarly, diamonds are cut so that light entering the stone strikes internal facets above the critical angle (~24.4° for diamond–air), maximizing brilliance.
In underwater photography and marine biology, the critical angle for water–air (~48.6°) creates the bright circle known as Snell’s window, through which an underwater observer sees the entire above-water hemisphere compressed into a cone. Understanding this angle is essential for designing aquatic lighting systems and underwater cameras.
This calculator instantly computes the critical angle in both radians and degrees. It also checks whether total internal reflection is physically possible for your chosen pair of media, ensuring you always get a meaningful result.
The critical angle is derived from Snell’s law at the limiting condition where the refracted ray travels along the boundary surface:
$$n_1 \sin\theta_c = n_2 \sin 90^\circ = n_2$$
Solving for θc:
$$\theta_c = \arcsin\!\left(\frac{n_2}{n_1}\right)$$
This equation is valid only when n₁ > n₂. If n₁ ≤ n₂, the ratio n₂/n₁ ≥ 1 and the arcsine is undefined, meaning total internal reflection cannot occur—light always partly refracts into the second medium.
Steps:
The critical angle is displayed in both radians and degrees. A smaller critical angle means total internal reflection occurs more easily—less tilting of the light ray is needed. For instance, diamond has a very small critical angle (~24.4°) compared to glass (~41.8°), which is why diamond sparkles more dramatically. If the calculator reports TIR Possible = 0, it means n₁ ≤ n₂ and no critical angle exists for that pair of media.
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Results
Crown glass (n₁ = 1.50) to air (n₂ = 1.00). The critical angle is about 41.8°. Any ray hitting the surface at an angle greater than 41.8° from the normal undergoes total internal reflection.
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Diamond (n₁ = 2.417) to air. The critical angle is only 24.4°, which is why diamond traps light internally and produces intense sparkle (brilliance).
Total internal reflection (TIR) occurs when a light ray traveling in a denser medium hits the boundary with a less dense medium at an angle of incidence greater than the critical angle. Instead of refracting through the boundary, 100% of the light is reflected back into the denser medium. TIR is the operating principle behind optical fibers and many prism-based optical instruments.
The critical angle formula θc = arcsin(n₂/n₁) requires the argument of the arcsine to be less than or equal to 1. This is only satisfied when n₁ > n₂. Physically, when light goes from a less dense to a denser medium, it bends toward the normal and can always partially refract—TIR never occurs.
Water has a refractive index of about 1.333. The critical angle for water–air is arcsin(1.0/1.333) ≈ 48.6°. This creates the phenomenon known as Snell’s window: an underwater observer sees the entire above-water world compressed into a bright circle subtending about 97.2°.
An optical fiber has a glass core with a higher refractive index surrounded by cladding with a lower index. Light injected into the core at angles exceeding the critical angle undergoes repeated total internal reflection, bouncing along the fiber with almost no energy loss. This allows signals to travel hundreds of kilometers.
Yes. Because the refractive index of most materials varies with wavelength (dispersion), the critical angle also varies slightly with wavelength. Shorter wavelengths (blue/violet) typically have a higher refractive index in glass, resulting in a slightly smaller critical angle compared to longer wavelengths (red).
Yes. TIR is not exclusive to light. Sound waves and seismic waves can also undergo total internal reflection when they pass from a medium where they travel more slowly into one where they travel faster. The same critical angle formula applies, using the ratio of wave speeds instead of refractive indices.
Roboculator Team
The Roboculator Team explains calculations, planning tools, and practical formulas in clear language for real-life situations.
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