Sorry this is just not possible as it would violate many of the basic rules of thermodynamics.
Hmm,I have a different view on this.There may be a possibility.When heat is converted to work or rather energy ,E=mc2 definitely comes in play.Then there is a particular(although small) mass change taking place.Thus if a engine on calculation shows that efficiency less than 100% it neve takes into account Quantum changes.These changes in course of a infinite number of times convert into significant energy. Thus at some point of time the efiiciency may go past 100% but only for a fraction of a second.Thus theoritically a deep look at it may say that the founder although joking may not be wrong.
non --- Evaporation is reversible by condensation, lowering the temperature.
The Carnot cycle gives the theoretical maximum efficiency of an engine operating between two heat reservoirs. The Carnot cycle is an idealized engine cycle that is thermodynamically reversible. Real systems such as power plants are not reversible, and the entropy of a real material changes with temperature (which is not accounted for by the Carnot cycle). A steam power plant operates closer to a cycle known as the Rankine cycle.
In a closed container at normal temperature it is reversible but at high temperature it is irreversible reaction.
Self locking machine has efficiency less than 50% but reversible machines has efficiency more than 50%
carnot cycle is the highiest efficiency
Enzymes are permanently inactivated by high temperature extremes. They are denatured.
Kinetic energy can be reconverted into potantial energy, but not with 100% efficiency. Some energe is lost in the process.
It's reversible. When you raise the temperature of frozen mercury, it 'melts' back into liquid form (just like ice melts back into water when you warm it).
explain why phase changes are reversible for solid to liquid and gas to liquid
reversible
No. All processes involving heat transfer are not reversible, since they result in an increase in entropy. Isothermal expansion implies heat transfer to maintain the system at a constant temperature. Normally an expanding gas would cool if there were no heat entering the system. Adiabatic processes involve no heat transfer and are reversible. The temperature can (and usually does) change during an adiabatic process.
A heat engine operating between 2 temperatures, Thot, the heat source, and Tcold, the heat sink, can be 100% efficient only when Tcold is absolute zero. Carnot worked out the equation to determine the best possible efficiency of a heat engine designed to produce mechanical energy ("Work") from heat energy: Wout = (Heat Energy in at Thot) x (Thot - Tcold)/(Thot) Note that (Thot - Tcold)/(Thot) is 1 only if Tcold is zero. In every other case, the ratio is less than 1. The amount of heat energy discharged to the heat sink at Tcold is: (Heat Energy in at Thot) - Wout. (You can work this out from the equation. It reflects the law of conservation of energy. ) This just means that all the heat energy absorbed by the heat engine is converted into either mechanical energy or heat energy at a lower temperature. No energy is lost and no extra energy is created. "Efficiency" according to Carnot's equation tells us the best possible ratio between these two energy outputs that nature allows a heat engine to achieve. You can think of a heat engine as a device that splits an amount of heat energy at some high temperature into mechanical energy and heat energy at some lower temperature. Kind Regards, Colin Dunstan Author: "cyclic heat to work conversion systems"