This post is part of a series,Nonsense and the Second Law of Thermodynamics The previous post is entitled Partition Functions.
The posts in this series are primarily about the second law of thermodynamics, the concept of entropy, and the use and abuse of these ideas. I would be remiss, however, not to mention information theory and the role that entropy plays. This post is not intended to be a comprehensive introduction to information theory. Readers especially interested in this topic will want to read other sources in addition to this post.
Topics
9/11
Acquisition Reform
Advertising
Alaway
Alcohol
Ale
Allergies
Antisemitism
Barack H. Obama
Beer
Billiards
Biology
Books
Budget
Bureaucracy
California
Capitalism
Carbohydrates
Carcinogen
CDC
Chemical Warfare
Chemistry
Chemophobia
Chirality
Climate Science
Colonial Pines
Computers
Conservation Laws
Constitution
Consumerism
Cosmology
CPT Invariance
Creationism
Customer Service
Daesh
David Irving
Dead End
Defense
Dinosaurs
Disasters
Economic
Energy
English
Ethics
Evolution
Fluoride
Food
FTL
Garden Care
George W. Bush
Gerlich and Tscheuschner
GISS
Glaciers
GMOs
HadCRU
Haiti
Health
Himalayan Rock Salt
HITRAN
Holocaust Denial
Home Brewing
How It Looks From Here
html
Humor
Information
Infrared Spectroscopy
IPCC
Iran
ISIS
Islam
Islamophobia
Israel
Ketotifen Fumarate
Law
Lawn Care
Leibniz
Lisbon
Magnetism
Math
Medco
Medicine
Modeling
Molecules
Monopoly
Monsanto
Naphazoline hydrochloride
Neutrinos
Nietzsche
NIH
NIST
Noether's Theorem
Non-hazardous
Norton Ghost
Nuclear Warfare
Oil
Oil Spill
Olopatadine hydrochloride
Opinion
Orson Scott Card
Parody
Pataday
Patanol
Pesticides
Pheneramine maleate
Physics
Plumbing
Politics
Poll
Pope
POTUS
Prescriptions
Prop 65
Psychology
Quantum Mechanics
Quiz
Racism
Radiative Transfer
Relativity
Religion
Respiration
Senior Housing
Signs
Smoking
Specific Gravity
Statistics
Stock Market
Sugars
Sun Tzu
Surface Temperature
Surgeon General
Symantec
Target
Temperature
Terrorism
The Final Solution
The Holocaust History Project
Thermodynamics
Time
Trains
Units
Voltaire
von Clausewitz
Weather
White House
Wine
Yeast
Friday, March 4, 2011
Friday, January 14, 2011
Temperature Anomalies and Graphing Data
Globally Averaged Temperature Anomaly
One statistic that is used to understand climate is the annual globally averaged temperature anomaly. It is not the only measure of global warming; there are a great many others, but it is one that the media tend to focus on because it is a convenient way of explaining what is happening to surface temperatures as a function of time.
The data here are taken from Global Land-Ocean Temperature Index (C) (Anomaly with Base: 1951-1980), which includes data from 1882-2007. There are updated numbers available for more recent years, but I am using these data to respond to an argument made by a friend.
One statistic that is used to understand climate is the annual globally averaged temperature anomaly. It is not the only measure of global warming; there are a great many others, but it is one that the media tend to focus on because it is a convenient way of explaining what is happening to surface temperatures as a function of time.
The data here are taken from Global Land-Ocean Temperature Index (C) (Anomaly with Base: 1951-1980), which includes data from 1882-2007. There are updated numbers available for more recent years, but I am using these data to respond to an argument made by a friend.
Sunday, January 2, 2011
Partition Functions
This post is part of a series,Nonsense and the Second Law of Thermodynamics. The previous post is entitled Fluctuations.
In previous posts it was shown that entropy is related to the the number of ways that a system can arrange itself subject to constraints such as constant energy.
The previous post on fluctuations showed that for very large numbers that fluctuation from the most probable distribution, are insignificant. Most of the distribution is contained within the square root of N of the most probable result.
In previous posts it was shown that entropy is related to the the number of ways that a system can arrange itself subject to constraints such as constant energy.
The previous post on fluctuations showed that for very large numbers that fluctuation from the most probable distribution, are insignificant. Most of the distribution is contained within the square root of N of the most probable result.
Friday, December 10, 2010
Carbon Dioxide Poll
A recently closed poll on this blog posed the following question. "The bending mode of carbon dioxide is:" Respondents were to respond with the best answer. Here were the choices:
- A Hoax
- Not Dipole Allowed
- Degenerate
- A Blackbody
- The reason the sky is blue
- Even though I understand Global Warming, I don't know
- I don't know
Friday, November 12, 2010
Fluctuations
This post is part of a series,Nonsense and the Second Law of Thermodynamics The previous post is entitled Entropy and Statistical Dynamics.
The second law of thermodynamics works because of the statistics of very large numbers. Consider a bouncing ball: as it bounces, it dissipates heat and eventually does not bounce as high.
The second law of thermodynamics works because of the statistics of very large numbers. Consider a bouncing ball: as it bounces, it dissipates heat and eventually does not bounce as high.

Saturday, November 6, 2010
Entropy and Statistical Thermodynamics
This post is part of a series, Nonsense and the Second Law of Thermodynamics. The previous post is entitled The Second Law and Swamp Coolers.
A previous post discusses the macroscopic thermodynamic definition of entropy, but there is another, statistical way of describing entropy. Consider an isolated macroscopic system of interacting molecules. Without knowing much about what is going on with the individual molecules, it is possible to measure macroscopic thermodynamic properties such as the pressure, the temperature etc.
(Figure Source)
Consider that the system is isolated; so that the total energy of the entire system of molecules is a constant. Energy is free to move from one molecule to another, and each molecule has multiple electronic, vibrational, rotational, and translational energy states that it could be in. There are many distinguishable ways that the system could be arranged to achieve the this energy.
A previous post discusses the macroscopic thermodynamic definition of entropy, but there is another, statistical way of describing entropy. Consider an isolated macroscopic system of interacting molecules. Without knowing much about what is going on with the individual molecules, it is possible to measure macroscopic thermodynamic properties such as the pressure, the temperature etc.
Consider that the system is isolated; so that the total energy of the entire system of molecules is a constant. Energy is free to move from one molecule to another, and each molecule has multiple electronic, vibrational, rotational, and translational energy states that it could be in. There are many distinguishable ways that the system could be arranged to achieve the this energy.
Saturday, October 30, 2010
The Second Law and Swamp Coolers
This post is part of a series, Nonsense and the Second Law of Thermodynamics. The previous post is entitled Heat Can Be Transferred From a Cold Body to a Hot Body: The Air Conditioner.
When I was an undergraduate, I had a physical chemistry professor who claimed that air conditioners that were completely inside a room could not possibly work. Opening the refrigerator door on a hot day will not make your house cooler.
The refrigerator gives off more heat than it transfers from inside itself; a refrigerator is actually heating the house. If the door is left open, the refrigerator works harder to try to maintain a cool temperature in accordance with its thermostat setting. As the refrigerator works harder, it releases more heat into the house.
My professor, however, was not correct. It is possible to have a cooling unit that does more cooling than it releases heat to the environment. The trick with indoor coolers is that the process by which they operate is not cyclic.
When I was an undergraduate, I had a physical chemistry professor who claimed that air conditioners that were completely inside a room could not possibly work. Opening the refrigerator door on a hot day will not make your house cooler.
The refrigerator gives off more heat than it transfers from inside itself; a refrigerator is actually heating the house. If the door is left open, the refrigerator works harder to try to maintain a cool temperature in accordance with its thermostat setting. As the refrigerator works harder, it releases more heat into the house.
My professor, however, was not correct. It is possible to have a cooling unit that does more cooling than it releases heat to the environment. The trick with indoor coolers is that the process by which they operate is not cyclic.
Subscribe to:
Posts (Atom)



