Question

Consider a black sphere of radius $R$ at temperature $T$ which radiates to distant black surroundings at $T=0 \mathrm{~K}$. (a) Surround the sphere with a nearby heat shield in the form of a black shell whose temperature is determined by radiative equilibrium. What is the temperature of the shell and what is the effect of the shell on the total power radiated to the surroundings? (b) How is the total power radiated affected by additional heat shields?

   Consider a black sphere of radius $R$ at temperature $T$ which radiates to distant black surroundings at $T=0 \mathrm{~K}$.
(a) Surround the sphere with a nearby heat shield in the form of a black shell whose temperature is determined by radiative equilibrium. What is the temperature of the shell and what is the effect of the shell on the total power radiated to the surroundings?
(b) How is the total power radiated affected by additional heat shields?
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Problems and Solutions on Thermodynamics and Statistical Mechanics
Problems and Solutions on Thermodynamics and Statistical Mechanics
U.S.T. of China… 1st Edition
Chapter 1, Problem 23 ↓

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According to the Stefan-Boltzmann law, the power radiated by the sphere is given by: \[ P_{\text{sphere}} = \sigma A T^4 = \sigma (4\pi R^2) T^4 \] where \( \sigma \) is the Stefan-Boltzmann constant and \( A \) is the surface area of the sphere.  Show more…

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Consider a black sphere of radius $R$ at temperature $T$ which radiates to distant black surroundings at $T=0 \mathrm{~K}$. (a) Surround the sphere with a nearby heat shield in the form of a black shell whose temperature is determined by radiative equilibrium. What is the temperature of the shell and what is the effect of the shell on the total power radiated to the surroundings? (b) How is the total power radiated affected by additional heat shields?
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Key Concepts

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Thermal Shielding
Thermal or heat shielding involves placing intermediate layers between a heat source and its surroundings to modify the temperature profile and radiative flux without altering the net power ultimately emitted into the environment. Although adding such shields changes the local temperatures (and can lead to lower temperatures at the shield surfaces), the overall energy balance in radiative equilibrium ensures that the power radiated to a much colder or zero-temperature environment remains determined by the original thermal source according to the Stefan-Boltzmann law.
Radiative Equilibrium
Radiative equilibrium occurs when the amount of energy absorbed by a body is exactly balanced by the energy it emits. In multi-layer systems such as those involving heat shields, each layer adjusts its temperature until the energy exchange between layers leads to a steady state, ensuring that the net heat flow is zero at each intermediate surface.
Stefan-Boltzmann Law
This law states that the total power emitted per unit area by a black surface is proportional to the fourth power of its absolute temperature (P/A = ?T^4). It is a key relation used to relate temperature with radiative flux in any system where thermal radiation is the dominant energy transfer mechanism.
Blackbody Radiation
This concept refers to an idealized object that absorbs all incident electromagnetic radiation, regardless of frequency or angle of incidence, and re-emits energy in a characteristic spectrum that depends solely on its temperature. Blackbody radiation is described by Planck's law and provides the basis for understanding thermal emission processes.

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