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Body Physics: Motion to Metabolism: Thermal Radiation Spectra

Body Physics: Motion to Metabolism
Thermal Radiation Spectra
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table of contents
  1. Cover
  2. Title Page
  3. Copyright
  4. Dedication
  5. Table Of Contents
  6. Why Use Body Physics?
  7. When to use Body Physics
  8. How to use Body Physics
  9. Tasks Remaining and Coming Improvements
  10. Who Created Body Physics?
  11. Unit 1: Purpose and Preparation
    1. The Body's Purpose
    2. The Purpose of This Texbook
    3. Prepare to Overcome Barriers
    4. Prepare to Struggle
    5. Prepare Your Expectations
    6. Prepare Your Strategy
    7. Prepare Your Schedule
    8. Unit 1 Review
    9. Unit 1 Practice and Assessment
  12. Unit 2: Measuring the Body
    1. Jolene's Migraines
    2. The Scientific Process
    3. Scientific Models
    4. Measuring Heart Rate
    5. Heart Beats Per Lifetime
    6. Human Dimensions
    7. Body Surface Area
    8. Dosage Calculations
    9. Unit 2 Review
    10. Unit 2 Practice and Assessment
  13. Unit 3: Errors in Body Composition Measurement
    1. Body Mass Index
    2. The Skinfold Method
    3. Pupillary Distance Self-Measurement
    4. Working with Uncertainties
    5. Other Methods of Reporting Uncertainty*
    6. Unit 3 Review
    7. Unit 3 Practice and Assessment
  14. Unit 4: Better Body Composition Measurement
    1. Body Density
    2. Body Volume by Displacement
    3. Body Weight
    4. Measuring Body Weight
    5. Body Density from Displacement and Weight
    6. Under Water Weight
    7. Hydrostatic Weighing
    8. Unit 4 Review
    9. Unit 4 Practice and Assessment
  15. Unit 5: Maintaining Balance
    1. Balance
    2. Center of Gravity
    3. Supporting the Body
    4. Slipping
    5. Friction in Joints
    6. Tipping
    7. Human Stability
    8. Tripping
    9. Types of Stability
    10. The Anti-Gravity Lean
    11. Unit 5 Review
    12. Unit 5 Practice and Assessment
  16. Unit 6: Strength and Elasticity of the Body
    1. Body Levers
    2. Forces in the Elbow Joint
    3. Ultimate Strength of the Human Femur
    4. Elasticity of the Body
    5. Deformation of Tissues
    6. Brittle Bones
    7. Equilibrium Torque and Tension in the Bicep*
    8. Alternative Method for Calculating Torque and Tension*
    9. Unit 6 Review
    10. Unit 6 Practice and Assessment
  17. Unit 7: The Body in Motion
    1. Falling
    2. Drag Forces on the Body
    3. Physical Model for Terminal Velocity
    4. Analyzing Motion
    5. Accelerated Motion
    6. Accelerating the Body
    7. Graphing Motion
    8. Quantitative Motion Analysis
    9. Falling Injuries
    10. Numerical Simulation of Skydiving Motion*
    11. Unit 7 Review
    12. Unit 7 Practice and Assessment
  18. Unit 8: Locomotion
    1. Overcoming Inertia
    2. Locomotion
    3. Locomotion Injuries
    4. Collisions
    5. Explosions, Jets, and Rockets
    6. Safety Technology
    7. Crumple Zones
    8. Unit 8 Review
    9. Unit 8 Practice and Assessment
  19. Unit 9: Powering the Body
    1. Doing Work
    2. Jumping
    3. Surviving a Fall
    4. Powering the Body
    5. Efficiency of the Human Body
    6. Weightlessness*
    7. Comparing Work-Energy and Energy Conservation*
    8. Unit 9 Review
    9. Unit 9 Practice and Assessment
  20. Unit 10: Body Heat and The Fight for Life
    1. Homeostasis, Hypothermia, and Heatstroke
    2. Measuring Body Temperature
    3. Preventing Hypothermia
    4. Cotton Kills
    5. Wind-Chill Factor
    6. Space Blankets
    7. Thermal Radiation Spectra
    8. Cold Weather Survival Time
    9. Preventing Hyperthermia
    10. Heat Death
    11. Unit 10 Review
    12. Unit 10 Practice and Assessment Exercises
  21. Laboratory Activities
    1. Unit 2/3 Lab: Testing a Terminal Speed Hypothesis
    2. Unit 4 Lab: Hydrostatic Weighing
    3. Unit 5 Lab: Friction Forces and Equilibrium
    4. Unit 6 Lab: Elastic Modulus and Ultimate Strength
    5. Unit 7 Lab: Accelerated Motion
    6. Unit 8 Lab: Collisions
    7. Unit 9 Lab: Energy in Explosions
    8. Unit 10 Lab: Mechanisms of Heat Transfer
  22. Design-Build-Test Projects
    1. Scale Biophysical Dead-lift Model
    2. Biophysical Model of the Arm
    3. Mars Lander
  23. Glossary

94

Thermal Radiation Spectra

The Electromagnetic Spectrum

Different names are used for electromagnetic radiation (light waves) with various ranges of frequency: radio waves, microwaves, infrared radiation, visible light, ultraviolet radiation, X-rays, and gamma rays. Collectively these ranges of frequencies make up the electromagnetic spectrum shown in the following diagram. The range frequencies that we can see is known as the visible spectrum, and we perceive the different frequencies within the visible spectrum as different colors. The wavelength of light, or any wave, is the distance between successive crests (peaks) of the wave. The frequency and wavelength of light waves are directly related and we can sometimes more easily relate to wavelength by comparing it to the length of familiar objects, so we often use wavelength instead of frequency to describe colors and the electromagnetic spectrum as a whole.

The electromagnetic spectrum. “EM Spectrum Properties reflected” by Inductiveload, via Wikimedia Commons

[1]

We can summarize the previous diagram in tabular form:

The previous diagram in tabular form
Radiation Type Wavelength (m)Approximate Wavelength ScaleFrequency (Hz)Temperature of object with thermal radiation peak at this wavelength (K)Significant penetration through atmosphere ?
Gamma Ray10-12Atomic Nucli1020No
X-ray10-10Atoms101810,000,000No
Ultraviolet (UV)10-8Molecules1016No (more at longer wavelength)
Visible0.5-6Protozoans101510,000Yes
Infrared (IR)10-5Needle Point1012100Yes (less at longer wavelength)
Microwave10-2Butterflies1081No
Radio103Humans to Buildings104Yes (less at shorter wavelength)

Black Body Radiation

A theoretically perfect emitter for which the emissivity is one (epsilon = 1) is known as black body emitter, because such an emitter would also be a perfect absorber and would thus appear completely black. The shape amount of light emitted at each wavelength defines the emission spectrum of the black body, which depends only on temperature in a well-defined way:

This graph shows the variation of blackbody Radiation intensity with wavelengths expressed in micrometers. Five curves that correspond to 2000 K, 3000 K, 4000 K, and 5000 K are drawn. The maximum of the radiation intensity shifts to the short-wavelength side with increase in temperature. It is in in the far-infrared for 2000 K, near infrared for 3000 K, red part of the visible spectrum for 4000 K, and green part of the visible spectrum for 5000 K.
The intensity of black body radiation plotted against the wavelength of the emitted radiation. Each curve corresponds to a different black body temperature, starting with a low temperature (the lowest curve) to a high temperature (the highest curve). Image Credit:  OpenStax University Physics Volume 3.

[2]

This simulations allows you to see how the black body emission spectrum depends on temperature:

Blackbody Spectrum

Exercises

An interactive or media element has been excluded from this version of the text. You can view it online here:
https://openoregon.pressbooks.pub/bodyphysics/?p=3152

We are often able to approximate the temperature of objects by assuming they are black body emitters and matching up their emission spectrum with that of  a black body with a known temperature. This is the basic principle behind thermal imaging cameras and handheld infrared (IR) thermometers such as the one in the following image. (Note that IR thermometers are often include a low power laser to improve aim, but contrary to popular belief, the laser is not involved in the temperature measurement).

A person points a hand-held, non-contact thermometer at the forehead of another person.
Contact tracers at a hospital in Conakry, Guinea demonstrate how to use a ThermoFlash infrared thermometer to monitor the temperatures of people who have come in contact with Ebola patients. Contacts are monitored for 21 days so that they can be isolated and treated as soon as possible if they develop symptoms. Image Credit: Infrared thermometer training by CDC Global via Wikimedia Commons.

[3]

For example, we can estimate the surface temperature of the sun to be roughly 6000  K (10,000 °F) because the actual emission spectrum of the Sun best matches the black body emission spectrum of an object at  6000  K, as seen in the following graph. Notice that the peak of the Sun’s emission spectrum is in the visible range, but that significant radiation power is found in the UV and IR regions. The UV light is capable of penetrating the dead out layer of skin (epidermis) and breaking some molecular bonds in your cells, including those in DNA, which can lead to sunburn and increased risk of skin cancer.

This graph shows the variation of blackbody Radiation intensity with wavelengths expressed in micrometers. The radiation curve of the sun (measured above the atmosphere is shown to agree very well with a curve corresponding to black body radiation from an object with temperature of 5777 K. The visible region of the spectrum is highlighted to show that the radiation curve of the sun is peaked in the visible region.
Emission spectrum of the sun as measured above the Earth’s atmosphere (AM0) compared to the black body spectrum of an object at 5777 K. Image Credit: Solar AM0 spectrum with visible spectrum background (en) by Danmichaelo [Public domain], from Wikimedia Commons

Everyday Example: Incandescent vs LED and Fluorescent Light Bulbs

Incandescent light bulbs use thermal radiation to generate light. In order for their emission spectrum to contain significant visible light their temperature must be several thousand Kelvin, as seen from the previous graph showing black body emission spectra at several temperatures. Temperatures of 3000 K to 4000 K are achieved by running electric current through the narrow filaments of inside the bulbs to cause resistive heating (conversion of electric potential energy to thermal energy). The filaments are made of high temperature tolerant metals like tungsten to prevent melting. Additionally, the majority of air within the bulb has been removed to prevent conduction and natural convection from heating the glass and to prevent the filaments from quickly oxidizing (rusting). The emission spectra for objects at 3000 K to 4000 K show us that much of their radiated power is in the IR range rather than the visible range, and thus doesn’t provide useful illumination. Consequently,  much of the electrical energy used to power incandescent light bulbs goes to waste. In fact, glass does absorb IR radiation so much of the wasted energy simply goes into making the bulb glass hot, in some cases dangerously so. Fluorescent and LED bulbs don’t use thermal radiation to generate light. Instead they apply voltages to energize electric charges trapped in atoms or in semi-conductor materials. When the electrons de-energize they emitted light at specific wavelengths, reducing the wasteful production of non-visible light. However, light from incandescent bulbs is sometimes considered more pleasing because it more closely resembles the emission spectrum of fire.

Dangerously Hot Cars

Some materials are transparent to visible light, but readily absorb IR light (notice how glasses prevent IR light from reaching the camera in this thermal image). Liquid water, water vapor, carbon dioxide (CO2) gas and most types of glass behave this way.  The emission spectrum of the sun shown above has significant emission in the UV, visible, and IR parts of the electromagnetic spectrum.  The visible light gets through the glass, which is why the glass appears transparent to you. The majority of UV is absorbed or reflected, preventing you from getting sunburn inside the car. The glass absorbs much of the IR light, which is re-radiated in both directions, in and out of the car. The visible light that gets through is partially absorbed by the interior of the car (especially if the interior is dark). That absorbed visible light is then re-radiated as IR light because the interior of the car is not nearly hot to enough to radiate visible light like the sun. That re-radiated IR light is absorbed by the glass and re-radiated again in both directions, in and out of the car. Therefore a significant portion of the incoming visible light energy gets trapped inside the car and the interior temperature can rise quickly, even if the outside air temperature is cool.  Green houses use this same phenomenon to keep plants warm in cool weather, so this phenomenon is commonly known as the green house effect.  It’s never a good idea to leave children or pets in cars. Even if you perform thoughtful calculations to predict the interior temperature for a given set of conditions such as air temperature, wind speed, and cloudiness, those conditions can change quickly.  It’s best not to risk injury to loved ones.

The Greenhouse Gas Effect

The Earth’s atmosphere acts like a car’s windshield. The atmosphere lets most UV and visible light through, but significant IR light is absorbed, primarily by water vapor and carbon dioxide gas. With respect to the Earth, this green-house effect is known as the Green House Gas Effect because the phenomenon is caused by gasses in the atmosphere instead of glass or plastic.

Figure shows UV, IR and visible light from the sun striking the earth through its atmosphere. Of these, only IR is reflected.
Illustration of the green house gas effect. UV, visible, and some IR light pass through the atmosphere. The UV and visible light are largely transformed to IR light. Only some of that IR light is able to escape back into space, the rest is trapped and the energy it contains increases the Earth’s average temperature. Image Credit: OpenStax University Physics.

[4]

The green house gas effect helps to keep the Earth’s temperature about 40 °C warmer than it would be without an atmosphere, which is a generally a good thing for us because most water on Earth would be frozen otherwise. Humans have established our modern infrastructure in accordance with the global climate that was present over the last few hundred years, but emission of carbon dioxide and methane (and other greenhouse gases) into Earth’s atmosphere from human activities strengthens the green house gas effect and increases the average temperature of the Earth.  Higher temperature means more thermal energy is available to drive more powerful convection cells and other thermodynamic processes that define weather and climate. The resulting changes in global climate are likely to cause a variety of dangerous and expensive consequences such as higher storm intensity, rising sea levels, and increased flooding in certain areas with prolonged drought in others.[5][6]
The following simulation allows you to examine how the green house gas effect works.

The Greenhouse Effect

Click to Run

  1. "EM Spectrum Properties reflected" by Inductiveload [CC BY-SA 3.0 (https://creativecommons.org/licenses/by-sa/3.0)], via Wikimedia Commons↵
  2. OpenStax University Physics, University Physics Volume 3. OpenStax CNX. Nov 12, 2018 http://cnx.org/contents/af275420-6050-4707-995c-57b9cc13c358@10.14. ↵
  3. Infrared thermometer training by CDC Global [CC BY 2.0 (https://creativecommons.org/licenses/by/2.0)], via Wikimedia Commons↵
  4. OpenStax University Physics, University Physics. OpenStax CNX. Oct 6, 2016 http://cnx.org/contents/74fd2873-157d-4392-bf01-2fccab830f2c@1.585↵
  5. "Fourth National Climate Assessment" by U.S. Global Change Research Program↵
  6. OpenStax University Physics, University Physics. OpenStax CNX. Oct 6, 2016 http://cnx.org/contents/74fd2873-157d-4392-bf01-2fccab830f2c@1.585↵

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Copyright © 2020 by Lawrence Davis. Body Physics: Motion to Metabolism by Lawrence Davis is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International License, except where otherwise noted.
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