Editing Heat engine (section)

== Enhancements ==
Engineers have studied the various heat-engine cycles to improve the amount of usable work they could extract from a given power source. The Carnot cycle limit cannot be reached with any gas-based cycle, but engineers have found at least two ways to bypass that limit and one way to get better efficiency without bending any rules:
#Increase the temperature difference in the heat engine. The simplest way to do this is to increase the hot side temperature, which is the approach used in modern combined-cycle [[gas turbine]]s. Unfortunately, physical limits (such as the melting point of the materials used to build the engine) and environmental concerns regarding [[NOx|NO<sub>x</sub>]] production (if the heat source is combustion with ambient air) restrict the maximum temperature on workable heat-engines. Modern gas turbines run at temperatures as high as possible within the range of temperatures necessary to maintain acceptable NO<sub>x</sub> output {{Citation needed|date=January 2010}}. Another way of increasing efficiency is to lower the output temperature. One new method of doing so is to use mixed chemical working fluids, then exploit the changing behavior of the mixtures. One of the most famous is the so-called [[Kalina cycle]], which uses a 70/30 mix of [[ammonia]] and water as its working fluid. This mixture allows the cycle to generate useful power at considerably lower temperatures than most other processes.
#Exploit the [[physical property|physical properties]] of the working fluid. The most common such exploitation is the use of water above the critical point ([[supercritical water]]). The behavior of fluids above their [[critical point (thermodynamics)|critical point]] changes radically, and with materials such as water and [[carbon dioxide]] it is possible to exploit those changes in behavior to extract greater thermodynamic efficiency from the heat engine, even if it is using a fairly conventional Brayton or Rankine cycle. A newer and very promising material for such applications is [[supercritical carbon dioxide|supercritical CO<sub>2</sub>]]. [[Sulfur dioxide|SO<sub>2</sub>]] and [[xenon]] have also been considered for such applications. Downsides include issues of corrosion and erosion, the different chemical behavior above and below the critical point, the needed high pressures and – in the case of sulfur dioxide and to a lesser extent carbon dioxide – toxicity. Among the mentioned compounds xenon is least suitable for use in a nuclear reactor due to the high [[neutron absorption]] cross section of almost all [[isotopes of xenon]], whereas carbon dioxide and water can also double as a [[neutron moderator]] for a thermal spectrum reactor.
#Exploit the [[chemical property|chemical properties]] of the working fluid. A fairly new and novel exploit is to use exotic working fluids with advantageous chemical properties. One such is [[nitrogen dioxide]] (NO<sub>2</sub>), a toxic component of smog, which has a natural [[dimer (chemistry)|dimer]] as di-nitrogen tetraoxide (N<sub>2</sub>O<sub>4</sub>). At low temperature, the N<sub>2</sub>O<sub>4</sub> is compressed and then heated. The increasing temperature causes each N<sub>2</sub>O<sub>4</sub> to break apart into two NO<sub>2</sub> molecules. This lowers the molecular weight of the working fluid, which drastically increases the efficiency of the cycle. Once the NO<sub>2</sub> has expanded through the turbine, it is cooled by the [[Thermal reservoir|heat sink]], which makes it recombine into N<sub>2</sub>O<sub>4</sub>. This is then fed back by the compressor for another cycle. Such species as [[aluminium bromide]] (Al<sub>2</sub>Br<sub>6</sub>), NOCl, and Ga<sub>2</sub>I<sub>6</sub> have all been investigated for such uses. To date, their drawbacks have not warranted their use, despite the efficiency gains that can be realized.<ref>{{cite web |url=https://netfiles.uiuc.edu/mragheb/www/NPRE%20402%20ME%20405%20Nuclear%20Power%20Engineering/Nuclear%20Reactors%20Concepts%20and%20Thermodynamic%20Cycles.pdf |title=Nuclear Reactors Concepts and Thermodynamic Cycles |access-date=2012-03-22 |url-status=dead |archive-url=https://web.archive.org/web/20090318233007/https://netfiles.uiuc.edu/mragheb/www/NPRE%20402%20ME%20405%20Nuclear%20Power%20Engineering/Nuclear%20Reactors%20Concepts%20and%20Thermodynamic%20Cycles.pdf |archive-date=18 March 2009}}</ref>