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Ice and water

In Section 41 it was shown that attraction between two dipoles in the vapour state can lead to the formation of double molecules. This phenomenon is called association and is observed with water, acetic acid and other substances containing a polar OH group. [Pg.176]

It still has to be explained why the boiling points of NH3 and HF are not also high. This is due to the fact that water, with its two positive poles, can easily form a lattice, whereas HF molecules, with only one positive and one negative pole in each, can at most only form chains or rings. In ammonia, which has three positive poles, a structure similar to that of water cannot be formed and it is again apparent that it is only a very special combination of circumstances which gives rise to the properties of water. [Pg.178]

The least distance to which the ion and dipole can approach each other is equal to the sum of the radii of the two. If a value of 3 A is assumed for this, then the energy is [Pg.178]


Shen Y R 1998 Sum frequency generation for vibrational spectroscopy applications to water interfaces and films of water and ice Solid State Commun. 108 399... [Pg.320]

Thermodynamic and physical properties of water vapor, Hquid water, and ice I are given ia Tables 3—5. The extremely high heat of vaporization, relatively low heat of fusion, and the unusual values of the other thermodynamic properties, including melting poiat, boiling poiat, and heat capacity, can be explained by the presence of hydrogen bonding (2,7). [Pg.209]

Pedden, T. M. Drinking Water and Ice Supplies and Their Relations to Health and Disease, G. P. Putnam s Sons, The Knickerbocker Press, New York, 1981... [Pg.58]

Vapor Pressure of Water and Ice and Calculation of Humid Air State Values 71... [Pg.41]

A mixture of 100 g of this solid and 1 liter of acetic anhydride was stirred and heated under reflux for 1.5 hours and then allowed to stand for 18 hours at room temperature. The excess acetic anhydride was removed in vacuo, and the residue was treated with one liter of water and ice and sufficient sodium bicarbonate to make neutral. The solid was collected, sucked dry on the filter, and triturated with hot ethanol. The ethanol solution on cooling gave 30.8 g of 4-acetyl-7-chloro-1,2,3,4-tetrahydro-1-methyl-5H-1,4-benzodiaze-pin-5-one. [Pg.909]

Glasel, J. A. Nuclear Magnetic Resonance Studies on Water and Ice, in Water — a Comprehensive Treatise, Vol. 1, chapter 6, New York, Plenum Press 1972... [Pg.33]

Point A on a phase diagram is the only one at which all three phases, liquid, solid, and vapor, are in equilibrium with each other. It is called the triple point. For water, the triplepoint temperature is 0.01°C. At this temperature, liquid water and ice have the same vapor pressure, 4.56 mm Hg. [Pg.233]

Self-Test 6.1A Water expands when it freezes. How much work does 100. g of water do when it freezes at 0°C and bursts a water pipe that exerts an opposing pressure of 1070 atm The densities of water and ice at 0°C are 1.00 g-cm 3 and 0.92 g-cm 3, respectively. [Pg.341]

Paper read at Royal Society meeting on Physics of Water and Ice , November... [Pg.441]

To survive freezing, a cell must be cooled in such a way that it contains little or no freezable water by the time it reaches the temperature at which internal ice formation becomes possible. Above that temperature, the plasma membrane is a barrier to the movement of ice crystals into the cytoplasm. The critical factor is the cooling rate. Even in the presence of external ice, most cells remain unfrozen, and hence, supercooled, 10 to 30 degrees below their actual freezing point (-0.5 °C in mammalian cells). Supercooled cell water has a higher chemical potential than that of the water and ice in the external medium, and as a consequence, it tends to flow out of the cells osmotically and freeze externally (Figure 1). [Pg.358]

As diagrammed in Figure 14-5. ice melts spontaneously if a mixture of water and ice is placed on a table at 25 °C H2 O (.S 0 ° Table top, 25 C 0 ° C) Recall from Section 11- that a phase change from solid to... [Pg.977]

Schematic view of the spontaneous process for a water-and-ice mixture on a table. The energy-absorbing process, melting, is spontaneous under these conditions. Schematic view of the spontaneous process for a water-and-ice mixture on a table. The energy-absorbing process, melting, is spontaneous under these conditions.
New York University. Water and Ice. Available online. URL http //www.nyu.edu/pages/mathmol/textbook/info water. html. [Pg.127]

Recognizing Cause and Effect If the mass remains constant for the water and ice but the volume changes, explain how this will affect the density. [Pg.24]

At present the Earth s temperature is not in thermal equilibrium, i.e., the net OLR is still not as high as generated net heat. Natural cold sinks in water, ground, and atmosphere slow down the effect of thermal pollution. The main sources of natural cold are in water and ice. The total volume of global water is 1.4 x 1018 m3, of which 94% is seawater while 3 x 1016 m3 (2%) of the water is ice in the form of glaciers and ice fields (Singh and Singh, 2001). [Pg.81]

Pure water is colorless, odorless, and tasteless. The earth is pretty much a closed system, neither gaining nor losing much water, with very little of the earth s water escaping into outer space thus, the same water that existed on the planet millions of years ago is still here. Water is, however, continually changing its form between water vapor, liquid water and ice, and moving around through, below, and above the surface of the earth (see Fig. 86). [Pg.437]

Although it is very hard to observe the absorption spectrum of eh when metal is dissolved in water because of its high reactivity, some attempts were made in water and ice (Jortner and Stein, 1955 Benett et al., 1964, 1967). Furthermore ESR (electron spin resonance) studies revealed that the trapped or solvated electron in ice interacts with six equivalent protons, thus ruling out H20-. [Pg.148]

Some reactions of aromatic compounds in water and methanol and of certain other compounds in water and ice have comparable specific rates. Due to considerable differences in solvation energies of both reactants and products, a transition state would require different barriers against reaction. [Pg.191]

Ice is a solid form of water, and is its only stable form below 0 °C. The liquid form of H20 is the only stable form in the temperature range 0 < T < 100 °C. Above 100 °C, the normal, stable phase is gaseous water, steam . Water s normal melting temperature 7(meit) is 0°C (273.15 K). The word normal in this context implies at standard pressure p . The pressure has a value of 105 Pa. This temperature T tneiu is often called the melting point because water and ice coexist indefinitely at this temperature and pressure, but at no other temperature can they coexist. We say they reside together at equilibrium. [Pg.178]

Figure 5.1 Schematic phase diagram showing pressures and temperatures at which two phases are at equilibrium. Phase boundary (a) represents the equilibrium between steam and ice boundary (b) represents equilibrium between water and ice and boundary (c) represents equilibrium between water and steam. The point D represents p and I on a warm, sunny day. Inset warming an ice cube from — 5 °C to the mouth at 37 °C at constant pressure causes the stable phase to convert from solid to liquid. The phase change occurs at 0 °C at... Figure 5.1 Schematic phase diagram showing pressures and temperatures at which two phases are at equilibrium. Phase boundary (a) represents the equilibrium between steam and ice boundary (b) represents equilibrium between water and ice and boundary (c) represents equilibrium between water and steam. The point D represents p and I on a warm, sunny day. Inset warming an ice cube from — 5 °C to the mouth at 37 °C at constant pressure causes the stable phase to convert from solid to liquid. The phase change occurs at 0 °C at...
Alternatively, try The colours of water and ice , by Terence Quickenden and Andrew Hanlon, Chemistry in Britain, December 2000, p. 37. [Pg.561]

Fennema, O. 1996. Water and ice. In Food Chemistry (O. Fennema, ed.). Dekker, New York. Finney, J.L. 2001. The water molecule and its interactions The interaction between theory, modeling and experiment. J. Mol. Liquids 90, 303-312. [Pg.92]


See other pages where Ice and water is mentioned: [Pg.272]    [Pg.396]    [Pg.143]    [Pg.144]    [Pg.396]    [Pg.141]    [Pg.33]    [Pg.340]    [Pg.382]    [Pg.997]    [Pg.3]    [Pg.415]    [Pg.797]    [Pg.254]    [Pg.96]    [Pg.300]    [Pg.21]    [Pg.24]    [Pg.4]    [Pg.434]    [Pg.55]    [Pg.15]    [Pg.181]    [Pg.16]   
See also in sourсe #XX -- [ Pg.176 ]

See also in sourсe #XX -- [ Pg.13 , Pg.221 , Pg.222 , Pg.223 , Pg.224 , Pg.225 , Pg.226 , Pg.227 , Pg.228 , Pg.229 , Pg.230 , Pg.231 , Pg.232 , Pg.233 , Pg.234 , Pg.238 , Pg.239 , Pg.240 , Pg.241 , Pg.242 , Pg.243 ]




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Hydrogen bonds cause unusual water, ice, and hydrate properties

Interaction between the Ice-Water Interface and Antifreeze Proteins

Liquid Water and Ice

Liquid Water and the Ices

Physical Properties of Water and Ice

Properties of Ice and Supercooled Water

Skin Supersolidity of Water and Ice

Specific Heat of Water and Ice

Structure of water and ices

The structures of ice and water

Vapor pressure of water and ice

Water and Ice on Asteroids

Water and ice polymorphs

Water ice

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