Distribution of US millionaires for the year 2000. The data points for many scientists are far to the left of this graph. (Data from ref. 2, graphed using Gnumeric.) |
S = kB ln(Ω),where S is the system entropy, kB is the Boltzmann constant (1.38062 x 10-23 joule/kelvin), and ln(Ω) is the natural logarithm of the number of possible states that the system can have. Entropy is used as a modeling tool, since the principle of maximum entropy states that the probability distribution that best fits your data is the one with the largest entropy. There are no simple examples of this, other than using the binary entropy function to decide that a coin toss should be 50:50. It's sufficient to note that there are more than 250 papers posted on arXiv with "Maximum Entropy" in the title, including a 111 page Ph.D. dissertation.[3] An open access paper entitled, "Global Inequality in Energy Consumption from 1980 to 2010," has just appeared in the journal, Entropy.[5-7] This paper, which is written by the physicists, Scott Lawrence, Qin Liu, and Victor M. Yakovenko of the University of Maryland (College Park) examines the global per capita consumption of energy in 2010. The partitioning of energy for individuals, as seen in the graph below, follows the same type of exponential distribution we see for the distribution of wealth in the graph above.
Complementary cumulative probability distribution function for 2010 per capita global energy consumption. The exponential fit on this log-linear scale is a straight line. (Inset from fig. 3 of ref. 5.) |
Creeping Gini. The Gini coefficient of global income has nearly doubled in the last two centuries. (data from Wikipedia, graphed using Gnumeric.) |