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What is a blackbody? How do real bodies differ from blackbodies?

Short Answer

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Answer: Real bodies differ from blackbodies in terms of their absorptivity and emissivity. Blackbodies are perfect absorbers and emitters of radiation, while real bodies do not absorb all incoming radiation and do not emit radiation solely based on their temperature. Real bodies' absorptivity and emissivity depend on their material properties, surface condition, and the wavelength and direction of incoming radiation. Additionally, real bodies can be selective absorbers and emitters, deviating from the blackbody spectrum.

Step by step solution

01

Define a blackbody

A blackbody is an idealized object that absorbs all incoming electromagnetic radiation, regardless of its wavelength or direction. It also emits radiation with a distinct spectrum, known as the blackbody spectrum, which depends solely on its temperature. In other words, blackbodies are perfect absorbers and perfect emitters of radiation.
02

Explain the blackbody spectrum

When a blackbody is heated, it emits radiation across a range of wavelengths. The amount of energy emitted at each wavelength is given by Planck's radiation law. The peak of the blackbody spectrum, as well as the total energy emitted, shift to shorter wavelengths and higher intensities as temperature increases. This relationship is described by Wien's displacement law and the Stefan-Boltzmann law, respectively.
03

Describe graphite's closeness to a blackbody

The best real-world approximation of a blackbody is graphite. Various real-world materials have emissivities close to one but not exactly equal to one. Graphite, which has an emissivity of about 0.99, is considered to be the closest natural material to a blackbody due to its high absorptivity and emissivity.
04

Explain how real bodies differ from blackbodies

Real bodies differ from blackbodies in terms of their absorptivity and emissivity. In general, real bodies do not absorb all incoming radiation and do not emit radiation solely based on their temperature. A real body's absorptivity and emissivity depend on its material properties, surface condition, and the wavelength and direction of incoming radiation.
05

Discuss selective absorbers and emitters

Real bodies can also be more selective in the wavelengths they absorb and emit compared to blackbodies, which makes them deviate from the blackbody spectrum. Greenhouse gases, for example, selectively absorb and emit infrared radiation, causing what is known as the greenhouse effect. Similarly, certain materials exhibit strong absorption and emission characteristics in specific wavelength ranges, making them useful in applications such as solar thermal energy conversion and stealth technology. In summary, blackbodies are idealized objects that absorb and emit radiation perfectly based on their temperature, while real bodies have more complex behaviors in terms of their absorptivity and emissivity based on their material properties, surface condition, and the direction of incoming radiation.

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Key Concepts

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

Idealized Objects
In the fascinating world of physics, an idealized object is something that serves as a perfect model for understanding complex phenomena. One notable example of an idealized object is the blackbody.
A blackbody is designed to be the ultimate absorber and emitter of radiation. It perfectly absorbs all electromagnetic radiation, no matter the wavelength or direction it comes from.
This ability makes it a valuable concept in physics, as it helps scientists understand how objects emit radiation based on temperature alone. Even though such perfect absorbers do not exist in nature, the concept helps establish a baseline for comparing real-world objects to a theoretical model.
Idealized objects reduce the complexities of real-life interactions into something manageable and calculable, offering a foundation for more advanced exploration of thermodynamic and optical properties.
Emissivity
When discussing blackbodies and real bodies, the concept of emissivity plays a central role. Emissivity is a measure of how efficiently an object emits energy as thermal radiation compared to a blackbody at the same temperature.
Its value ranges from 0 to 1, with 1 indicating perfect emission, characteristic of an ideal blackbody. An object with high emissivity, like graphite, which has an emissivity close to 0.99, can almost perfectly emit thermal radiation.
Emissivity is significant in understanding heat transfer, as it can impact how an object radiates energy to its surroundings. This measurement is crucial in fields such as thermography, heating and cooling designs, and even climate modeling to comprehend how different materials release heat energy.
  • A perfect blackbody has an emissivity of 1.
  • Real-world objects generally have emissivities less than 1.
  • Emissivity affects how objects cool and heat up.
Absorptivity
Absorptivity is another important characteristic to consider when comparing real bodies with blackbodies. It measures how well an object absorbs radiation at a given wavelength.
For blackbodies, absorptivity is always at its maximum value of 1, meaning they absorb all incoming radiation perfectly. Real bodies, however, vary in how much radiation they absorb, depending on the material and surface texture.
This property is not only wavelength-dependent but also dependent on the angle of incidence. This variability in absorptivity can explain why some materials are better at heating up under sunlight, while others might remain cooler.
Understanding absorptivity helps in applications ranging from designing energy-efficient buildings to manufacturing clothing that can keep you warm or cool. The distinction between blackbodies and real bodies lies in how they handle incoming energy.
  • A blackbody's absorptivity equals 1.
  • Material properties influence real bodies' absorptivity.
  • Absorptivity impacts solar absorption and energy efficiency.
Real Bodies vs Blackbodies
Real bodies and blackbodies are often compared to illustrate the differences in how materials interact with electromagnetic radiation. While a blackbody is a theoretical construct that perfectly absorbs and emits radiation, real bodies exhibit different properties due to their material composition.
Real objects have emissivity and absorptivity values less than 1, meaning they neither absorb nor emit radiation perfectly.
These differences make real objects more selective in the wavelengths they absorb and emit, affecting a variety of natural and engineered processes. For instance, greenhouse gases selectively absorb infrared radiation, contributing to the greenhouse effect.
Furthermore, various materials can be engineered to focus on specific wavelengths for specific applications, such as in solar panels or thermal insulation. This selectivity introduces complexity in predicting behavior, contrasting sharply with the simplicity of blackbody assumptions.
  • Real bodies have limited emissivity and absorptivity.
  • Material and surface impact radiation interactions.
  • Selectivity leads to diverse real-world applications.

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Most popular questions from this chapter

Determine a positive real root of this equation using \(E E S\) : $$ 3.5 x^{3}-10 x^{0.5}-3 x=-4 $$

Heat is lost steadily through a \(0.5-\mathrm{cm}\) thick \(2 \mathrm{~m} \times 3 \mathrm{~m}\) window glass whose thermal conductivity is \(0.7 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The inner and outer surface temperatures of the glass are measured to be \(12^{\circ} \mathrm{C}\) to \(9^{\circ} \mathrm{C}\). The rate of heat loss by conduction through the glass is (a) \(420 \mathrm{~W}\) (b) \(5040 \mathrm{~W}\) (c) \(17,600 \mathrm{~W}\) (d) \(1256 \mathrm{~W}\) (e) \(2520 \mathrm{~W}\)

Four power transistors, each dissipating \(12 \mathrm{~W}\), are mounted on a thin vertical aluminum plate \(22 \mathrm{~cm} \times 22 \mathrm{~cm}\) in size. The heat generated by the transistors is to be dissipated by both surfaces of the plate to the surrounding air at \(25^{\circ} \mathrm{C}\), which is blown over the plate by a fan. The entire plate can be assumed to be nearly isothermal, and the exposed surface area of the transistor can be taken to be equal to its base area. If the average convection heat transfer coefficient is \(25 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), determine the temperature of the aluminum plate. Disregard any radiation effects.

In a power plant, pipes transporting superheated vapor are very common. Superheated vapor is flowing at a rate of \(0.3 \mathrm{~kg} / \mathrm{s}\) inside a pipe with \(5 \mathrm{~cm}\) in diameter and \(10 \mathrm{~m}\) in length. The pipe is located in a power plant at \(20^{\circ} \mathrm{C}\), and has a uniform pipe surface temperature of \(100^{\circ} \mathrm{C}\). If the temperature drop between the inlet and exit of the pipe is \(30^{\circ} \mathrm{C}\), and the specific heat of the vapor is \(2190 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\), determine the heat transfer coefficient as a result of convection between the pipe surface and the surrounding.

Two surfaces, one highly polished and the other heavily oxidized, are found to be emitting the same amount of energy per unit area. The highly polished surface has an emissivity of \(0.1\) at \(1070^{\circ} \mathrm{C}\), while the emissivity of the heavily oxidized surface is \(0.78\). Determine the temperature of the heavily oxidized surface.

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