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This tutorial visualizes blackbody radiation: an ideal emitter whose spectrum depends only on temperature. You can see how total power radiated grows as P ∝ T4 (Stefan-Boltzmann), how the peak wavelength shifts with λmax ∝ 1/T (Wien's law), and how the object's apparent color follows the Planckian locus from dull red to blue-white.
Mathematical foundation1. Stefan-Boltzmann law Total power radiated per unit area: P = σ A T4, where σ ≈ 5.67×10−8 W/(m²·K4). Doubling the temperature T increases power by a factor of 24 = 16. 2. Planck's law Spectral radiance (power per unit area, solid angle, and wavelength): L(λ,T) = (2hc²/λ⁵) / (ehc/(λkT) − 1). The graph plots this curve; the area under it is related to total power. 3. Wien's displacement law Peak wavelength: λmax = b / T, with b ≈ 2.898×10−3 m·K. Hotter objects peak at shorter (bluer) wavelengths. The dashed line on the graph shows λmax. 4. Color (Planckian locus) The color of the "emitter" circle approximates the chromaticity of a blackbody at that temperature: red → orange → yellow → white → blue-white as T increases. Stefan-Boltzmann Lab3000 KTotal radiance P = σ T4: Peak wavelength λmax: Doubling T → 16× power. Tutorial: hue visible at all T Emitter (Planckian color) Spectral radiance vs wavelength. Shaded band: visible (380–700 nm). Dashed line: Wien λmax. Overlay: auto-X (max X where Y < 5% of peak), comp (compare curves), Lin/Log (X-axis scale).
UsageDrag the Temperature slider from 300 K to 10,000 K:
Lab ideas1. Stefan-Boltzmann: Note the "Total radiance" value. Double the temperature (e.g. 3000 K → 6000 K) and confirm the power increases by about 16×. 2. Wien's law: At 3000 K the peak is in the infrared (~966 nm). At 6000 K it moves to ~483 nm (visible). At 10,000 K it is in the UV (~290 nm). 3. Color: Compare 800 K (dim red), 3000 K (orange-white), 6000 K (sun-like white), 10,000 K (blue-white).
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