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Today we'll explore thermal radiation, which is energy emitted by matter due to its temperature. Unlike conduction and convection, thermal radiation doesnβt require a medium to travel, and it moves at the speed of light. Can anyone tell me what that means for our daily observations of heat?
Does that mean we feel heat from the sun even when there's nothing between us?
Exactly! That's a perfect example. The sun emits radiation that reaches us in a vacuum. Now, letβs discuss the modes of interaction: absorption, reflection, and transmission. What do you think happens when we touch a hot surface?
We get burned because our skin absorbs the heat!
Great point, Student_2! And what about something that feels cold despite being in a hot room?
It reflects the heat instead of absorbing it!
Exactly! Absorbed heat affects our temperature, while reflected heat does not. Letβs remember this with the acronym 'ART' β Absorption, Reflection, Transmission.
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Now, let's discuss some critical terms: emissivity, absorptivity, reflectivity, and transmissivity. Who can help define emissivity?
Itβs the ratio of radiation emitted by a surface to that of a blackbody at the same temperature!
Well done! And what about absorptivity?
Itβs the fraction of incident radiation absorbed by a material.
Correct! How would we relate these properties for opaque surfaces?
By saying that absorptivity plus reflectivity equals one!
Right! Keep in mind this equation: Ξ± + Ο = 1. Now think about non-opaque materials, how would that change?
We would also need to consider transmissivity, so it becomes Ξ± + Ο + Ο = 1.
Excellent participation! Just remember 'ART' applies to both opaque and non-opaque materials.
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Next, weβll explore the Stefan-Boltzmann Law, which states that the blackbody emissive power is described by the equation E_b = ΟTβ΄. Who can tell me what Ο represents?
That would be the Stefan-Boltzmann constant!
Great! And what does the 'T' stand for?
Itβs the absolute temperature in Kelvin!
Exactly! So, how does a real surface differ in terms of emissive power?
Itβs multiplied by the emissivity factor, right? E = Ξ΅ΟTβ΄.
Correct! Remember, emissivity indicates how different real surfaces will behave compared to an ideal blackbody. Itβs very crucial in engineering applications.
Can you give us an example of where this is applied?
Sure! Itβs applicable in industries like aerospace where thermal management is vital. Now, letβs recap: the Stefan-Boltzmann Law is fundamental in understanding radiative heat transfer.
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Now letβs distinguish between blackbody and greybody. What's the definition of a blackbody?
A blackbody is an ideal emitter and absorber at Ξ΅ = 1.
Correct! And what about a greybody?
A greybody has Ξ΅ less than 1, meaning itβs a real surface that doesnβt emit or absorb as perfectly as a blackbody.
Exactly! Now, why is it important to understand the difference?
Because it helps us predict how different materials will behave in terms of heat radiation.
Well said! Remember, blackbodies are theoretical while greybodies apply to real-life materials. This sets the stage for analyzing multiple body exchanges.
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Next, weβll learn about radiation heat transfer between surfaces! The formula is q12 = Ο(T14 - T24) / (...) What do you think this equation accounts for?
It considers surface emissivity and geometry!
Exactly! The equation also incorporates view or shape factors. Who can recall the importance of view factors?
They describe how much radiation from one surface strikes another!
Perfect! View factors are crucial in thermal analysis. This section makes sure we understand how geometry impacts radiative heat transfer.
Are there practical applications for this?
Yes! It's widely used in furnace designs and spacecraft thermal insulation. Remember, the principles we covered apply systematically across various heat transfer scenarios.
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Radiative Properties of materials are explored, highlighting key concepts such as emissivity, absorptivity, reflectivity, and transmissivity. Additionally, the section discusses the StefanβBoltzmann Law and differentiates between blackbody and greybody radiation, emphasizing their significance in radiation heat transfer.
This section delves into the principles of radiative properties that govern how materials interact with thermal radiation. Key concepts covered include:
The section also outlines the StefanβBoltzmann Law, providing the relationship governing blackbody radiation, which shows that the emissive power of a blackbody is directly related to the fourth power of its absolute temperature. Furthermore, the distinction between blackbody (Ξ΅ = 1) and greybody (Ξ΅ < 1) radiation is discussed along with practical applications for these concepts in multiple surface interactions through view factors, radiosity methods, and the use of radiation shields. This knowledge is critical for applications in thermal systems such as furnaces and spacecraft design.
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β Emissivity (Ξ΅B):
β Ratio of radiation emitted by a surface to that by a blackbody at the same temperature
Emissivity is a measure of how effectively a surface emits thermal radiation compared to an ideal blackbody at the same temperature. A blackbody is a perfect emitter with an emissivity of 1. Therefore, if a surface has an emissivity of 0.9, it means that it emits 90% of the thermal radiation that a blackbody would emit at the same temperature. Emissivity values can range from 0 to 1.
Imagine you have two pots on the stove, one made of black cast iron and the other made of shiny stainless steel. The cast iron pot has a higher emissivity (it emits heat better) than the shiny stainless steel pot. Even if both pots are at the same temperature, the cast iron pot will radiate heat more effectively than the stainless steel pot.
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b. Absorptivity (Ξ±B):
β Fraction of incident radiation absorbed
Absorptivity refers to the proportion of incoming radiation that is absorbed by a surface. If a material has an absorptivity of 0.7, it means that 70% of the incoming radiation is absorbed, while the remaining 30% may be reflected or transmitted. This property is crucial for materials used in solar collectors, where maximizing absorption is desired.
Think about wearing a black T-shirt on a sunny day compared to wearing a white one. The black T-shirt absorbs more sunlight (radiation) and gets hotter, while the white T-shirt reflects more sunlight and stays cooler. This is a practical manifestation of absorptivity in everyday life.
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c. Reflectivity (ΟB):
β Fraction of incident radiation reflected
Reflectivity is defined as the fraction of incident radiation that is reflected off a surface. A surface with a high reflectivity reflects most of the radiation that hits it, which is particularly useful in applications where heat loss needs to be minimized, such as in building materials aiming to keep interiors cool.
Consider a mirror. When you look into it, almost all of the light (radiation) that hits the mirror is reflected back to you. This high level of reflectivity makes mirrors ideal for various applications, from decoration to telescopes, where capturing and redirecting light is essential.
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d. Transmissivity (ΟB):
β For non-opaque materials: Ξ±+Ο+Ο=1
Transmissivity is the fraction of incident radiation that passes through a material. For non-opaque materials, the sum of absorptivity (Ξ±), reflectivity (Ο), and transmissivity (Ο) must equal 1 (i.e., Ξ± + Ο + Ο = 1). This means if a surface absorbs 40% and reflects 30%, then it must transmit 30% of the incident radiation.
Think of a window. When sunlight hits it, a portion of the light gets absorbed by the glass, some is reflected, and the rest passes through, allowing light into your room. The transmissivity of the glass determines how much light gets through. Clear glass has high transmissivity, while tinted or frosted glass has lower transmissivity.
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Key Concepts
Emissivity: The measure of a surface's ability to emit thermal radiation.
Absorptivity: Determines how much incident radiation is absorbed by a material.
Reflectivity: The portion of incident radiation that is reflected.
Transmissivity: Determines how much radiation passes through a material.
Stefan-Boltzmann Law: A fundamental relationship for blackbody radiation, linking emissive power to temperature.
Black and Grey Bodies: Ideal vs. real-world surfaces regarding radiation properties.
View Factors: Important for calculating radiative heat transfer between surfaces.
See how the concepts apply in real-world scenarios to understand their practical implications.
A black oven emulates a black body, absorbing all light and heat, maximizing cooking efficiency.
In a spacecraft, surfaces must be carefully designed with appropriate emissivities to manage extreme temperature fluctuations in space.
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In the heat we feel, with radiation so real, it travels far and wide, no medium to hide.
Imagine two friends, one wearing a black coat, absorbing the sunβs rays, while the other wears a white coat, reflecting most of the heat. This shows how emissivity and reflectivity change their experiences in the sun.
Remember 'A-R-T' for Absorptivity, Reflectivity, and Transmissivity - key players in how surfaces behave with radiation!
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Review the Definitions for terms.
Term: Emissivity (Ξ΅)
Definition:
The ratio of radiation emitted by a surface to that of a blackbody at the same temperature.
Term: Absorptivity (Ξ±)
Definition:
The fraction of incident radiation absorbed by a surface.
Term: Reflectivity (Ο)
Definition:
The fraction of incident radiation that is reflected off a surface.
Term: Transmissivity (Ο)
Definition:
The fraction of incident radiation transmitted through a material.
Term: StefanBoltzmann Law
Definition:
A physical law that describes the power radiated by a blackbody in terms of its temperature.
Term: Blackbody
Definition:
An idealized object that perfectly absorbs all incident radiation at all wavelengths.
Term: Greybody
Definition:
A real surface that does not absorb or emit radiation perfectly, with an emissivity less than 1.
Term: View Factor (Fij)
Definition:
The proportion of radiation leaving surface i that strikes surface j.
Term: Radiosity (J)
Definition:
The total energy leaving a surface, including emitted and reflected energy.