000			03483nam a22005295i 4500
001			978-3-540-49901-5
003			DE-He213
005			20161121231201.0
007			cr nn 008mamaa
008			100301s2007 gw | s |||| 0|eng d
020			_a9783540499015 _9978-3-540-49901-5
024	7		_a10.1007/978-3-540-49901-5 _2doi
050		4	_aTJ265
050		4	_aQC319.8-338.5
072		7	_aTGMB _2bicssc
072		7	_aSCI065000 _2bisacsh
082	0	4	_a621.4021 _223
100	1		_aTerao, Kunio. _eauthor.
245	1	0	_aIrreversible Phenomena _h[electronic resource] : _bIgnitions, Combustion and Detonation Waves / _cby Kunio Terao.
264		1	_aBerlin, Heidelberg : _bSpringer Berlin Heidelberg, _c2007.
300			_aX, 409 p. _bonline resource.
336			_atext _btxt _2rdacontent
337			_acomputer _bc _2rdamedia
338			_aonline resource _bcr _2rdacarrier
347			_atext file _bPDF _2rda
505	0		_aClassical Ignition Theories -- Stochastic Theory of Irreversible Phenomena -- Nucleation in Phase Transition -- Shock Tubes -- Stochastic Ignition Theory -- Ignition in a Fuel Spray -- Ignition by Electric Sparks -- Nonequilibrium State -- Interaction Between Combustion and Pressure or Shock Waves -- Gaseous Detonation Waves -- Industrial Applications of Detonation Waves.
520			_aIdeals are simple and able to be easily understood, but never exist in reality. In this book a theory based on the second law of thermodynamics and its applications are described. In thermodynamics there is a concept of an ideal gas which satisfies a mathematical formula PV = RT. This formula can appro- mately be applied to the real gas, so far as the gas has not an especially high pressure and low temperature. In connection with the second law of thermo- namics there is also a concept of reversible and irreversible processes. The reversible process is a phenomenon proceeding at an infinitely low velocity, while the irreversible process is that proceeding with a finite velocity. Such a process with an infinitely slow velocity can really never take place, and all processes observed are always irreversible, therefore, the reversible process is an ideal process, while the irreversible process is a real process. According to the first law of thermodynamics the energy increase dU of the thermodynamic system is a sum of the heat dQ added to the system and work dW done in the system. Practically, however, the mathematical formula of the law is often expressed by the equation , or some similar equations derived from this formula, is applied to many phenomena. Such formulae are, however, th- retically only applicable to phenomena proceeding at an infinitely low velocity, that is, reversible processes or ideal processes.
650		0	_aEngineering.
650		0	_aPhysical chemistry.
650		0	_aContinuum physics.
650		0	_aThermodynamics.
650		0	_aHeat engineering.
650		0	_aHeat transfer.
650		0	_aMass transfer.
650		0	_aFluid mechanics.
650	1	4	_aEngineering.
650	2	4	_aEngineering Thermodynamics, Heat and Mass Transfer.
650	2	4	_aClassical Continuum Physics.
650	2	4	_aPhysical Chemistry.
650	2	4	_aEngineering Fluid Dynamics.
710	2		_aSpringerLink (Online service)
773	0		_tSpringer eBooks
776	0	8	_iPrinted edition: _z9783540499008
856	4	0	_uhttp://dx.doi.org/10.1007/978-3-540-49901-5
912			_aZDB-2-ENG
950			_aEngineering (Springer-11647)
999			_c509779 _d509779