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Leidenfrost effect
The Leidenfrost effect is a physical phenomenon in which a liquid, in near contact with a mass significantly hotter than the liquid's boiling point, produces an insulating vapor layer keeping that liquid from boiling rapidly. Due to this ‘repulsive force,’ the droplet hovers over the surface rather than making physical contact with it. This is most commonly seen when cooking; one sprinkles drops of water in a pan to gauge its temperature: if the pan's temperature is at or above the Leidenfrost point, the water skitters across the pan and takes longer to evaporate than in a pan below the temperature of the Leidenfrost point (but still above boiling temperature). The effect is also responsible for the ability of liquid nitrogen to skitter across floors. It has also been used in some potentially dangerous demonstrations, such as dipping a wet finger in molten lead[1] or blowing out a mouthful of liquid nitrogen, both enacted without injury to the demonstrator.[2] The latter is potentially lethal, particularly should one accidentally swallow the liquid nitrogen.[3]
It is named after Johann Gottlob Leidenfrost, who discussed it in A Tract About Some Qualities of Common Water in 1756.
Effect
Excitation of normal modes in a drop of water during the Leidenfrost effect
The effect can be seen as drops of water are sprinkled onto a pan at various times as it heats up. Initially, as the temperature of the pan is just below 100 °C (212 °F), the water flattens out and slowly evaporates, or if the temperature of the pan is well below 100 °C (212 °F), the water stays liquid. As the temperature of the pan goes above 100 °C (212 °F), the water droplets hiss when touching the pan and these droplets evaporate quickly. Later, as the temperature exceeds the Leidenfrost point, the Leidenfrost effect comes into play. On contact with the pan, the water droplets bunch up into small balls of water and skitter around, lasting much longer than when the temperature of the pan was lower. This effect works until a much higher temperature causes any further drops of water to evaporate too quickly to cause this effect.
This is because at temperatures above the Leidenfrost point, the bottom part of the water droplet vaporizes immediately on contact with the hot plate. The resulting gas suspends the rest of the water droplet just above it, preventing any further direct contact between the liquid water and the hot plate. As steam has much poorer thermal conductivity, further heat transfer between the pan and the droplet is slowed down dramatically. This also results in the drop being able to skid around the pan on the layer of gas just under it.
Behavior of water on a hot plate. Graph shows heat transfer (flux) vs temperature. Leidenfrost effect occurs after transition boiling.
The temperature at which the Leidenfrost effect begins to occur is not easy to predict. Even if the volume of the drop of liquid stays the same, the Leidenfrost point may be quite different, with a complicated dependence on the properties of the surface, as well as any impurities in the liquid. Some research has been conducted into a theoretical model of the system, but it is quite complicated.[4] As a very rough estimate, the Leidenfrost point for a drop of water on a frying pan might occur at 193 °C (379 °F).[citation needed]
The effect was also described by the eminent Victorian steam boiler designer, Sir William Fairbairn, in reference to its effect on massively reducing heat transfer from a hot iron surface to water, such as within a boiler. In a pair of lectures on boiler design,[5] he cited the work of Pierre Hippolyte Boutigny (1798-1884) and Professor Bowman of King's College, London in studying this. A drop of water that was vaporized almost immediately at 168 °C (334 °F) persisted for 152 seconds at 202 °C (396 °F). Lower temperatures in a boiler firebox might evaporate water more quickly as a result; compare Mpemba effect. An alternative approach was to increase the temperature beyond the Leidenfrost point. Fairbairn considered this too, and may have been contemplating the flash steam boiler, but considered the technical aspects insurmountable for the time.
The Leidenfrost point may also be taken to be the temperature for which the hovering droplet lasts longest.[6]
It has been demonstrated that it is possible to stabilize the Leidenfrost vapour layer of water by exploiting superhydrophobic surfaces. In this case, once the vapour layer is established, cooling never collapses the layer, and no nucleate boiling occurs; the layer instead slowly relaxes until the surface is cooled.[7]
Leidenfrost effect has been used for the development of high sensitivity ambient mass spectrometry. Under the influence of Leidenfrost condition the Levitating droplet does not release molecules out and the molecules are enriched inside the droplet. At the last moment of droplet evaporation all of the enriched molecules release in a short time domain and thus increase the sensitivity.[8]
A heat engine based on the Leidenfrost effect has been prototyped. It has the advantage of extremely low friction.[9]
Leidenfrost point
A water droplet experiencing Leidenfrost effect on a hot stove plate
The Leidenfrost point signifies the onset of stable film boiling. It represents the point on the boiling curve where the heat flux is at the minimum and the surface is completely covered by a vapor blanket. Heat transfer from the surface to the liquid occurs by conduction and radiation through the vapor. In 1756, Leidenfrost observed that water droplets supported by the vapor film slowly evaporate as they move about on the hot surface. As the surface temperature is increased, radiation through the vapor film becomes more significant and the heat flux increases with increasing excess temperature.
The minimum heat flux for a large horizontal plate can be derived from Zuber's equation,[6]
\( {{\frac{q}{A}}_{min}}=C{{h}_{fg}}{{\rho }_{v}}{{\left[ \frac{\sigma g\left( {{\rho }_{L}}-{{\rho }_{v}} \right)}{{{\left( {{\rho }_{L}}+{{\rho }_{v}} \right)}^{2}}} \right]}^{{}^{1}\!\!\diagup\!\!{}_{4}\;}} \)
where the properties are evaluated at saturation temperature. Zuber's constant, C is approximately 0.09 for most fluids at moderate pressures.
Heat transfer correlations
The heat transfer coefficient may be approximated using Bromley's equation,[6]
\( h=C{{\left[ \frac{k_{v}^{3}{{\rho }_{v}}g\left( {{\rho }_{L}}-{{\rho }_{v}} \right)\left( {{h}_{fg}}+0.4{{c}_{pv}}\left( {{T}_{s}}-{{T}_{sat}} \right) \right)}{{{D}_{o}}{{\mu }_{v}}\left( {{T}_{s}}-{{T}_{sat}} \right)} \right]}^{{}^{1}\!\!\diagup\!\!{}_{4}\;}} \)
Where, {{D}_{o}} is the outside diameter of the tube. The correlation constant C is 0.62 for horizontal cylinders and vertical plates and 0.67 for spheres. Vapor properties are evaluated at film temperature.
For stable film boiling on a horizontal surface, Berenson has modified Bromley's equation to yield,[10]
\(h=0.325{{\left[ \frac{k_{vf}^{3}{{\rho }_{vf}}g\left( {{\rho }_{L}}-{{\rho }_{v}} \right)\left( {{h}_{fg}}+0.4{{c}_{pv}}\left( {{T}_{s}}-{{T}_{sat}} \right) \right)}{{{\mu }_{vf}}\left( {{T}_{s}}-{{T}_{sat}} \right)\sqrt{\sigma /g\left( {{\rho }_{L}}-{{\rho }_{v}} \right)}} \right]}^{{}^{1}\!\!\diagup\!\!{}_{4}\;}} \)
For vertical tubes, Hsu and Westwater have correlated the following equation,[10]
\( h{{\left[ \frac{\mu _{v}^{2}}{g{{\rho }_{v}}\left( {{\rho }_{L}}-{{\rho }_{v}} \right)k_{v}^{3}} \right]}^{{}^{1}\!\!\diagup\!\!{}_{3}\;}}=0.0020{{\left[ \frac{4m}{\pi {{D}_{v}}{{\mu }_{v}}} \right]}^{0.6}} \)
Where, m is the mass flow rate in \( l{{b}_{m}}/hr \) at the upper end of the tube
At excess temperatures above that at the minimum heat flux, the contribution of radiation becomes appreciable and becomes dominant at high excess temperatures. The total heat transfer coefficient can be is thus a combination of the two. Bromley has suggested the following equations for film boiling boiling from the outer surface of horizontal tubes.
\({{h}^{{}^{4}\!\!\diagup\!\!{}_{3}\;}}={{h}_{conv}}^{{}^{4}\!\!\diagup\!\!{}_{3}\;}+{{h}_{rad}}{{h}^{{}^{1}\!\!\diagup\!\!{}_{3}\;}}
\)
\( 1\If {{h}_{rad}}<{{h}_{conv}}, \)
\( h={{h}_{conv}}+\frac{3}{4}{{h}_{rad}} \)
The effective radiation coefficient, \( {{h}_{rad}} \) can be expressed as,
\( {{h}_{rad}}=\frac{\varepsilon \sigma \left( T_{s}^{4}-T_{sat}^{4} \right)}{\left( {{T}_{s}}-{{T}_{sat}} \right)} \)
Where, \( \varepsilon \) is the emissivity of the solid and \sigma is the Stefan-Boltzmann constant.
The pressure field in a Leidenfrost droplet
The equation for the pressure field in the vapor region between the droplet and the solid surface can be solved for using the standard momentum and continuity equations. For the sake of simplicity in solving, a linear temperature profile and a parabolic velocity profile are assumed within the vapor phase. The heat transfer within the vapor phase is assumed to be through conduction. With these approximations, the Navier-Stokes equation can be solved[11] to get the pressure field.
Leidenfrost temperature and surface tension effects
The Leidenfrost temperature is the property of a given set of solid-liquid pair. The temperature of the solid surface beyond which the liquid undergoes Leidenfrost phenomenon is termed as Leidenfrost temperature. The calculation of Leidenfrost temperature involves the calculation of minimum film boiling temperature of a fluid. Berenson[12] obtained a relation for the minimum film boiling temperature from minimum heat flux arguments. While the equation for the minimum film boiling temperature, which can be found in the reference above, is quite complex, the features of it can be understood from a physical perspective. One critical parameter to consider is the surface tension. The proportional relationship between the minimum film boiling temperature and surface tension is to be expected since fluids with higher surface tension need higher quantities of heat flux for the onset of nucleate boiling. Since film boiling occurs after nucleate boiling, the minimum temperature for film boiling should have a proportional dependence on the surface tension.
Henry[13] developed a model for Leidenfrost phenomenon which includes transient wetting and microlayer evaporation. Since the Leidenfrost phenomenon is a special case of film boiling, the Leidenfrost temperature is related to the minimum film boiling temperature via a relation which factors in the properties of the solid being used. While the Leidenfrost temperature is not directly related to the surface tension of the fluid, it is indirectly dependent on it through the film boiling temperature. For fluids with similar thermophysical properties, the one with higher surface tension usually has a higher Leidenfrost temperature.
For example, for saturated water-copper interface, the Leidenfrost temperature is 257 °C (495 °F). The Leidenfrost temperatures for glycerol and common alcohols are significantly smaller due to their lower surface tension values (density and viscosity differences are also contributing factors.)
Reactive Leidenfrost effect
Reactive Leidenfrost effect of cellulose on silica, 750 °C (1,380 °F)
Non-volatile materials were discovered in 2015 to also exhibit a 'reactive Leidenfrost effect,' whereby solid particles were observed to float above hot surfaces and skitter around erratically.[14] Detailed characterization of the reactive Leidenfrost effect was completed for small particles of cellulose (~0.5 mm) on high temperature polished surfaces by high speed photography. Cellulose was shown to decompose to short-chain oligomers which melt and wet smooth surfaces with increasing heat transfer associated with increasing surface temperature. Above 675 °C (1,247 °F), cellulose was observed to exhibit transition boiling with violent bubbling and associated reduction in heat transfer. Liftoff of the cellulose droplet (depicted at the right) was observed to occur above about 750 °C (1,380 °F) associated with a dramatic reduction in heat transfer.[15] High speed photography of the reactive Leidenfrost effect of cellulose on porous surfaces (macroporous alumina) was also shown to suppress the reactive Leidenfrost effect and enhance overall heat transfer rates to the particle from the surface. The new phenomenon of a 'reactive Leidenfrost (RL) effect' was characterized by a dimensionless quantity (φRL= τconv/τrxn), which relates the time constant of solid particle heat transfer to the time constant of particle reaction, with the reactive Leidenfrost effect occurring for 10−1< φRL< 10+1. The reactive Leidenfrost effect with cellulose will occur in numerous high temperature applications with carbohydrate polymers including biomass conversion to biofuels, preparation and cooking of food, and tobacco use.[16]
In popular culture
In Jules Verne's 1876 book Michael Strogoff, the protagonist is saved from being blinded with a hot blade by evaporating tears.
In the 2009 season finale of MythBusters, "Mini Myth Mayhem", the team demonstrated that a person can wet their hand and briefly dip it into molten lead without injury, using the Leidenfrost effect as the scientific basis.
In the fourth episode of the anime Aldnoah.Zero, the effect is mentioned as the cause of bullet tips melting midair after contacting plasma and subsequently being veered off course by the wind surrounding them.
See also
Critical heat flux
Mpemba effect
Nucleate boiling
region-beta paradox
References
Willey, David (1999). "The Physics Behind Four Amazing Demonstrations". Skeptical Inquirer 23 (6). Retrieved 11 October 2014.
Walker, Jearl. "Boiling and the Leidenfrost Effect" (PDF). Fundamentals of Physics: 1–4. Retrieved 11 October 2014.
"Student Gulps Into Medical Literature". Worcester Polytechnic Institute. 20 January 1999. Retrieved 11 October 2014.
Bernardin, John D.; Mudawar, Issam (2002). "A Cavity Activation and Bubble Growth Model of the Leidenfrost Point". Journal of Heat Transfer 124 (5): 864–74. doi:10.1115/1.1470487.
Sir William Fairbairn (1851). Two Lectures: The Construction of Boilers, and on Boiler Explosions, with the means of prevention.[page needed]
Incropera, DeWitt, Bergman & Lavine: Fundamentals of Heat and Mass Transfer, 6th edition.[page needed]
Vakarelski, Ivan U.; Patankar, Neelesh A.; Marston, Jeremy O.; Chan, Derek Y. C.; Thoroddsen, Sigurdur T. (2012). "Stabilization of Leidenfrost vapour layer by textured superhydrophobic surfaces". Nature 489 (7415): 274–7. Bibcode:2012Natur.489..274V. doi:10.1038/nature11418. PMID 22972299.
Subhrakanti Saha, Lee Chuin Chen, Mridul Kanti Mandal, Kenzo Hiraoka (March 2013). "Leidenfrost Phenomenon-assisted Thermal Desorption (LPTD) and Its Application to Open Ion Sources at Atmospheric Pressure Mass Spectrometry". Journal of The American Society for Mass Spectrometry 3 (24): 341–7. doi:10.1007/s13361-012-0564-y.
Wells, Gary G.; Ledesma-Aguilar, Rodrigio; McHale, Glen; Sefiane, Khellil (3 March 2015). "A sublimation heat engine". Nature Communications. Bibcode:2015NatCo...6E6390W. doi:10.1038/ncomms7390. Retrieved 5 March 2015.
James R. Welty; Charles E. Wicks; Robert E. Wilson; Gregory L. Rorrer., "Fundamentals of Momentum, Heat and Mass transfer" 5th edition, John Wiley and Sons[page needed]
Carey, Van P. , Liquid Vapor Phase change Phenomena
Berenson, P.J., Film boiling heat transfer from a horizontal surface, Journal of Heat Transfer, Volume 83, 1961, Pages 351-362
Henry,R.E., [A correlation for the minimum film boiling temperature],Chem. Eng. Prog. Symp. Ser. , Volume 70, 1974, Pages 81-90
"Scientists levitate wood on structured surfaces captured by high speed photography" Phys.org. http://phys.org/news/2015-06-scientists-levitate-wood-surfaces-captured.html
"Reactive Liftoff of Crystalline Cellulose Particles", Scientific Reports 2015, 5, 11238. DOI: 10.1038/srep11238
Scientists Levitate Wood on Structured Surfaces Captured by High Speed Photography. http://www.newswire.com/press-release/scientists-levitate-wood-on-structured-surfaces-captured-by
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