Examples of isotropic in the following topics:
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- If the emitter is isotropic or the emitters are randomly oriented then the total power emitted per unit volume and unit frequency is
- Often the emission is isotropic and it is convenient to define the emissivity of the material per unit mass
- ϵν is simply related to jν for an isotropic emitter
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- For example, if you have an isotropic source, the flux is constant across a spherical surface centered on the source, so you find that
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- In this region, the radiation field is nearly isotropic, but it need not be close to a blackbody distribution.
- Because the intensity is close to isotropic we can approximate it by
- which we found earlier to hold for strictly isotropic radiation fields.
- The source function Sν is isotropic, so let's average the radiative transfer equation over direction to yield
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- Such substances that expand in all directions are called isotropic.
- For isotropic materials, the area and linear coefficients may be calculated from the volumetric coefficient (discussed below).
- For isotropic material, and for small expansions, the linear thermal expansion coefficient is one third the volumetric coefficient.
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- But let's assume that the radiation field is isotropic, so I=J for all directions, we get
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- If we assume that the photon distribution is isotropic, the angle ⟨cosθ⟩=0.
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- The factor of threes arise because we assume that the radiation is isotropic so the value of Ex2 is typically one third of E2 .
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- Let's suppose that we have an isotropic distribution of photons of a single energy E0 and a beam of electrons traveling along the x-axis with energy γmc2 and density N.
- Let's assume that there are many beams isotropically distributed, so we need to find the mean value of j(Ef,μf) over angle,
- To be more precise, we could have relaxed the assumption that the scattering is isotropic and we would have found
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