Based on the figure, at a temperature of 300 \(\mathrm{K}\) and a wavelength of \(30 \times 10^{-6} \mathrm{m}\) , the brightness of a black- body will most likely be: A. less than \(5 \times 10^{6}\) watts per \(\mathrm{m}^{3}\) and \(40 \times 10^{6}\) watts B. between \(5 \times 10^{6}\) watts per \(m^{3}\) and \(40 \times 10^{6}\) watts per \(m^{3}\) . C. between \(41 \times 10^{6}\) watts per \(m^{3}\) and \(130 \times 10^{6}\) watts per \(m^{3}\) . D. greater than \(130 \times 10^{6}\) watts per \(m^{3}\) .

Short Answer

Expert verified
Answer: The brightness of the black body is less than 5 x 10^6 watts per m^3 and 40 x 10^6 watts.

Step by step solution

01

Write down the Planck's law formula

The Planck's law formula is: \[ B(\lambda, T) = \frac{2\pi hc^2}{\lambda^5} \frac{1}{e^{\frac{hc}{\lambda k T}} - 1} \] where: - \(B(\lambda, T)\) is the brightness at wavelength \(\lambda\) and temperature \(T\) - \(h\) is the Planck's constant (\(6.626 \times 10^{-34} m^2kg/s\)) - \(c\) is the speed of light (\(3.00 \times 10^8 m/s\)) - \(k\) is the Boltzmann constant (\(1.381 \times 10^{-23} J/K\))
02

Plug in the values and calculate the brightness

Given, Temperature, \(T = 300 K\) Wavelength, \(\lambda = 30 \times 10^{-6} m\) Now let's plug these values into the Planck's law formula: \[ B(30 \times 10^{-6}, 300) = \frac{2\pi (6.626 \times 10^{-34})(3.00 \times 10^8)^2}{(30 \times 10^{-6})^5} \frac{1}{e^{\frac{(6.626 \times 10^{-34})(3.00 \times 10^8)}{(30 \times 10^{-6})(1.381 \times 10^{-23})(300)}} - 1} \] Solving this, we get the brightness \(B(30 \times 10^{-6}, 300) = 1.173 \times 10^6 \mathrm{W/m^3}\)
03

Compare the brightness to the given options

Now that we have calculated the brightness, let's compare it to the given options: A. less than \(5 \times 10^6\) watts per \(\mathrm{m}^3\) and \(40 \times 10^6\) watts B. between \(5 \times 10^6\) watts per \(m^3\) and \(40 \times 10^6\) watts per \(m^3\) C. between \(41 \times 10^6\) watts per \(m^{3}\) and \(130 \times 10^{6}\) watts per \(m^{3}\) D. greater than \(130 \times 10^{6}\) watts per \(m^{3}\) Since the calculated brightness, \(1.173 \times 10^6 \mathrm{W/m^3}\) is less than the range given in option A, the answer is: A. less than \(5 \times 10^6\) watts per \(\mathrm{m}^3\) and \(40 \times 10^6\) watts

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Black-Body Radiation
Black-body radiation is a fundamental concept in physics that describes the type of electromagnetic radiation emitted by an object that absorbs all the radiation that falls on it. A perfect black body is an idealized object that does not reflect or transmit any radiation, meaning it is a perfect absorber and equally a perfect emitter of radiation.

When an object is heated, it emits radiation over a wide range of wavelengths, but the intensity of radiation peaks at a particular wavelength dependent on the temperature of the object. This phenomenon is described by Planck's law, which provides the spectral distribution of a black body's emission enabling us to calculate the brightness for a given temperature and wavelength.

Understanding this concept helps in several practical applications, including thermal imaging, astrophysics to determine the temperature of stars and planets, and even climatology for understanding the Earth's radiation budget.
Planck's Constant
Planck's constant, denoted as \(h\), is a fundamental constant in physics that has the value \(6.626 \times 10^{-34} m^2kg/s\). It plays a crucial role in the field of quantum mechanics, representing the smallest action—effectively a 'quantum'—that can be observed in nature.

This constant is not only part of the Planck's law formula that describes the spectral brightness of black-body radiation, but it's also a key component of other quantum phenomena, including the energy of a photon, \(E = hu\), where \(u\) is the frequency of the radiation. Understanding Planck's constant is therefore essential for studying the interaction between matter and electromagnetic radiation at the smallest scales.
Boltzmann Constant
The Boltzmann constant \(k\), which is approximately equal to \(1.381 \times 10^{-23} J/K\), is a constant linking the average kinetic energy of particles in a gas with its temperature. This constant plays a fundamental role in statistical mechanics and thermodynamics, encapsulating how individual particle energies are distributed within a system.

In Planck's law formula, the Boltzmann constant is utilized as part of the exponential factor that determines the distribution of energy at different wavelengths for a given temperature. It's also a critical component of the ideal gas law and makes appearances in the entropy and Boltzmann distribution equations, reflecting its broad importance for understanding thermal properties of materials at the atomic and molecular levels.

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