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   Gases, Liquids, and Solids | 
 
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   Fig. 7.1	The water in the lake behind the dam has potential energy as a result
       of its position. | 
 
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   Fig. 7.3	(a) In a solid, the particles are close together. (b) In a liquid, the
       particles slide freely over one another. (c) In a gas, the particles are
       in random motion. | 
 
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   Fig. 7.4	Gas molecules can be compared to billiard balls in random motion,
       bouncing off one another. | 
 
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   Fig. 7.5	When a gas is compressed, the amount of empty space in the container is
       decreased. | 
 
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   Fig. 7.6	The essential components of a mercury barometer are a graduated glass
       tube, a glass dish, and liquid mercury. | 
 
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   Fig. 7.7	Robert Boyle was self-taught. Through his efforts, the true value of
       experimental investigation was first recognized. | 
 
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   Fig. 7.8	Data illustrating the inverse proportionality associated with Boyle’s
       law. | 
 
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   Fig. 7.9      When the volume of a
       gas at constant temperature decreases by half, the average number of
       times a molecule hits the container walls is doubled. | 
 
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   Fig. 7.10	Filling a syringe with a liquid is an application of Boyle’s law. | 
 
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   Fig. 7.11	Jacques Charles in the process of working with hot-air balloons made
       the observations that led to the formulation of what is now known as
       Charles’s law. | 
 
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   Fig. 7.12	Data illustrating the direct proportionality associated with Charles’s
       law. | 
 
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   Fig. 7.13	John Dalton had an interest in the study of weather. | 
 
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   Fig. 7.14 	                                                                                             
       A set of four containers can be used to illustrate Dalton’s law
       of partial pressures. The pressure in the fourth container equals the
       sum of the first three. | 
 
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   Fig. 7.15	There are six changes of state possible for substances. | 
 
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   The beaker contains iodine crystals. | 
 
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   Fig. 7.17	(a) the liquid level drops for a time, (b) then becomes constant. At
       that point a state of equilibrium has been reached in which (c) the rate
       of evaporation equals the rate of condensations. | 
 
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   Fig. 7.18	Bubbles of vapor form within a liquid when the temperature of the
       liquid reaches the liquid’s boiling point. | 
 
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   Fig. 7.19	The converse of the pressure cooker “phenomenon” is that food cooks
       more slowly at reduced pressure. | 
 
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   Fig. 7.20	There are many dipole-dipole interactions possible between randomly
       arranged CIF molecules. | 
 
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   Fig. 7.21	Depiction of hydrogen bonding among the water molecules. | 
 
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   Fig. 7.22	Diagrams of hydrogen bonding involving selected simple molecules. | 
 
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   Fig. 7.23	If there were no hydrogen bonding between water molecules, the boiling
       point of water would be approximately -80C.
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   Fig. 7.24	Nonpolar molecules can develop instantaneous dipoles and induced
       dipoles. | 
 
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