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  1. The emission spectrum of a blackbody can be obtained by analyzing the light radiating from the hole. Electromagnetic waves emitted by a blackbody are called blackbody radiation. Figure 6.2.2: The intensity of blackbody radiation versus the wavelength of the emitted radiation.

  2. namely that energy is emitted only in discrete energy values, or quants: En = nhν = nhc/λ, where n is an integer, h is a constant (later called Planck’s constant), c is the speed of light, ν is the frequency of radiation and λ is the wavelength.

  3. with Planck’s formula for radiation energy intensity in the same interval: ρ (f, T) Δ f = 8 π V f 2 Δ f c 3 h f e h f / k B T 1, for the low frequency modes h f ≪ k B T we can make the approximation e h f / k B T − 1 ≅ h f / k B T. and it follows immediately that each mode has energy k B T, in line with classical predictions ...

  4. The waves can exchange energy with the walls. The objective here is to find the energy density distribution among various modes of vibration at various wavelengths (or frequencies). In other words, we want to know how much energy is carried by a single wavelength or a band of wavelengths.

  5. Planck’s Derivation of the Energy Density of Blackbody Radiation. To calculate the number of modes of oscillation of electromagnetic radiation possible in a cavity, consider a one-dimensional box of side L. In equilibrium only standing waves are possible, and these will have nodes at the ends x = 0, L. and since =.

  6. General X-Ray Formulas. Wavelength and photon energy relationship: h! = hc = 1239:842 eV nm. Number of photons required for 1 joule of energy: 1 joule ) 5:034 1015 [nm] photons.

  7. Planck’s radiation law, a mathematical relationship formulated in 1900 by German physicist Max Planck to explain the spectral-energy distribution of radiation emitted by a blackbody (a hypothetical body that absorbs all radiant energy falling upon it).

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