{"id":7555,"date":"2021-06-08T21:56:46","date_gmt":"2021-06-08T21:56:46","guid":{"rendered":"https:\/\/opentextbc.ca\/introductorychemistry\/chapter\/properties-of-liquids\/"},"modified":"2021-10-04T19:01:51","modified_gmt":"2021-10-04T19:01:51","slug":"properties-of-liquids","status":"publish","type":"chapter","link":"https:\/\/opentextbc.ca\/introductorychemistry\/chapter\/properties-of-liquids\/","title":{"raw":"Properties of Liquids","rendered":"Properties of Liquids"},"content":{"raw":"
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Learning Objectives<\/p>\r\n\r\n<\/header>\r\n

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  1. Define the vapour pressure of liquids.<\/li>\r\n \t
  2. Explain the origin of both surface tension and capillary action.<\/li>\r\n<\/ol>\r\n<\/div>\r\n<\/div>\r\nThere are some properties that all liquids have. The liquid that we are most familiar with is probably water, and it has these properties. Other liquids have them as well, which is something to keep in mind.\r\n\r\nAll liquids have a certain portion of their particles having enough energy to enter the gas phase, and if these particles are at the surface of the liquid, they do so (see Figure 10.1 \"Evaporation\"). The formation of a gas from a liquid at temperatures below the boiling point is called evaporation<\/strong>. At these temperatures, the material in the gas phase is called vapour<\/strong>, rather than gas; the term gas<\/em> is reserved for when the gas phase is the stable phase.\r\n\r\n[caption id=\"attachment_7544\" align=\"aligncenter\" width=\"600\"]\"\" Figure 10.1 \"Evaporation.\" Some particles of a liquid have enough energy to escape the liquid phase to become a vapour.[\/caption]\r\n\r\nIf the available volume is large enough, eventually all the liquid will become vapour. But if the available volume is not enough, eventually some of the vapour particles will reenter the liquid phase (see Figure 10.2 \"Equilibrium\"). At some point, the number of particles entering the vapour phase will equal the number of particles leaving the vapour phase, so there is no net change in the amount of vapour in the system. We say that the system is at equilibrium<\/em>. The partial pressure of the vapour at equilibrium is called the vapour pressure of the liquid<\/em>.\r\n\r\n[caption id=\"attachment_7545\" align=\"aligncenter\" width=\"600\"]\"\" Figure 10.2 \"Equilibrium.\" At some point, the number of particles entering the vapour phase will be balanced by the number of particles returning to the liquid. This point is called equilibrium.[\/caption]\r\n\r\nUnderstand that the liquid has not stopped evaporating. The reverse process \u2014 condensation \u2014 is occurring as fast as evaporation is, so there is no net change in the amount of vapour in the system. The term dynamic equilibrium<\/strong>\u00a0represents a situation in which a process still occurs, but the opposite process also occurs at the same rate so that there is no net change in the system.\r\n\r\nThe vapour pressure for a substance is dependent on the temperature of the substance; as the temperature increases, so does the vapour pressure. Figure 10.3 \"Plots of Vapour Pressure versus Temperature for Several Liquids\" is a plot of vapour pressure versus temperature for several liquids. Having defined vapour pressure, we can also redefine the boiling point<\/em> of a liquid: the temperature at which the vapour pressure of a liquid equals the surrounding environmental pressure. The normal vapour pressure, then, is the temperature at which the vapour pressure is 760 torr, or exactly 1 atm. Thus boiling points vary with surrounding pressure, a fact that can have large implications on cooking foods at lower- or higher-than-normal elevations. Atmospheric pressure varies significantly with altitude.\r\n\r\n[caption id=\"attachment_7546\" align=\"aligncenter\" width=\"500\"]\"\" Figure 10.3 \"Plots of Vapour Pressure versus Temperature for Several Liquids.\" The vapour pressure of a liquid depends on the identity of the liquid and the temperature, as this plot shows.[\/caption]\r\n\r\n
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    Example 10.1<\/p>\r\n\r\n<\/header>\r\n

    \r\n\r\nUse Figure 10.3 \"Plots of Vapour Pressure versus Temperature for Several Liquids\" to estimate the boiling point of water at 500 torr, which is the approximate atmospheric pressure at the top of Mount Everest.\r\n\r\nSolution<\/em>\r\n\r\nSee the accompanying figure. Five hundred torr is between 400 and 600, so we extend a line from that point on the y<\/em>-axis across to the curve for water and then drop it down to the x<\/em>-axis to read the associated temperature. It looks like the point on the water vapour pressure curve corresponds to a temperature of about 90\u00b0C, so we conclude that the boiling point of water at 500 torr is 90\u00b0C.\r\n\r\n[caption id=\"attachment_7547\" align=\"aligncenter\" width=\"500\"]\"\" Figure 10.4 Using Figure 10.3 \"Plots of Vapour Pressure versus Temperature for Several Liquids\" to Answer Example 10.1[\/caption]\r\n\r\nBy reading the graph properly, you can estimate the boiling point of a liquid at different temperatures.\r\n\r\nTest Yourself<\/em>\r\n\r\nUse Figure 10.3 \"Plots of Vapour Pressure versus Temperature for Several Liquids\" to estimate the boiling point of ethanol at 400 torr.\r\n\r\nAnswer<\/em>\r\n\r\nAbout 65\u00b0C.\r\n\r\n<\/div>\r\n<\/div>\r\nThe vapour pressure curve for water is not exactly zero at the melting point \u2014 0\u00b0C. Even ice has a vapour pressure; that is why it sublimes over time. However, the vapour pressures of solids are typically much lower than that of liquids. At \u22121\u00b0C, the vapour pressure of ice is 4.2 torr. At a freezer temperature of 0\u00b0F (\u221217\u00b0C), the vapour pressure of ice is only 1.0 torr; so-called deep freezers can get down to \u221223\u00b0C, where the vapour pressure of ice is only 0.6 torr.\r\n

    Phase Diagrams<\/h1>\r\nA phase diagram is a graphical representation of the equilibrium relationships that exist between the phases of a substance under specified pressures and temperatures (see Figure 10.5 \u201cA generic phase diagram\u201d). The phase diagram is a combination of three curves: the vapour pressure curve, the melting curve and the sublimation curve. We have previously seen that vapour pressure curves represent the equilibrium between the liquid and gas phase, and the point at which the pressure equals 1 atm is the normal boiling point. One additional feature of this curve in the phase diagram (green), is that it ends at the critical point<\/strong>. The critical point is the point at the highest temperature and pressure at which liquids and gases remain distinguishable. At temperatures and pressure beyond this point the matter exists in a phase with properties of both liquids and gases known as a supercritical fluid<\/strong>.\r\n\r\nThe melting curve (orange) represents the equilibrium between solid and liquid, and the point at which the pressure equals 1 atm is the normal melting point. The sublimation curve (blue) represents the equilibrium which exists between solid and gas. Finally, the point where all three curves meet is known as the triple point. At this point, three phases (solid, liquid and gas) all exist at equilibrium.\r\n\r\n[caption id=\"attachment_587\" align=\"aligncenter\" width=\"600\"]\"A Figure 10.5 \"A generic phase diagram.\"[\/caption]\r\n\r\n
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    Example 10.2<\/p>\r\n\r\n<\/header>\r\n

    \r\n\r\nUsing the following phase diagram, determine what would happen if:\r\n
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    1. The temperature is increased for matter at point 1.<\/li>\r\n \t
    2. The pressure is increased for matter at point 3.<\/li>\r\n<\/ol>\r\n[caption id=\"attachment_588\" align=\"aligncenter\" width=\"400\"]\"example Figure 10.6 \"Example phase diagram.\"[\/caption]\r\n\r\nSolution<\/em>\r\n
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      1. Matter at point 1 will melt (change phase from solid to liquid) if the temperature is increased.<\/li>\r\n \t
      2. Matter at point 3\u00a0will condense\u00a0(change phase from gas\u00a0to liquid) if the temperature is increased.<\/li>\r\n<\/ol>\r\n<\/div>\r\n<\/div>\r\n

        Surface Tension and Capillary Action<\/h1>\r\nAll liquids share some other properties as well. Surface tension<\/strong>\u00a0is an effect caused by an imbalance of forces on the atoms at the surface of a liquid, as shown in Figure 10.7 \"Surface Tension\". The blue particle in the bulk of the liquid experiences intermolecular forces from all around, as illustrated by the arrows. However, the yellow particle on the surface does not experience any forces above it because there are no particles above it. This leads to an imbalance of forces that we call surface tension.\r\n\r\n[caption id=\"attachment_7550\" align=\"aligncenter\" width=\"600\"]\"\" Figure 10.7 \"Surface Tension.\" Surface tension comes from the fact that particles at the surface of a liquid do not experience interactions from all directions, leading to an imbalance of forces on the surface.[\/caption]\r\n\r\n[caption id=\"attachment_590\" align=\"aligncenter\" width=\"400\"]\"Water Figure 10.8 \"Effects of Surface Tension.\" Water on the surface of this apple beads up due to the effect of surface tension.[\/caption]\r\n\r\nSurface tension is responsible for several well-known behaviours of liquids, including water. Liquids with high surface tension tend to bead up when present in small amounts (Figure 10.8 \"Effects of Surface Tension\"). Surface tension causes liquids to form spheres in free fall or zero gravity (see Figure 10.16 \"Liquids and Gravity\"<\/a>: the \"floating\" water isn't in the shape of a sphere by accident; it is the result of surface tension). Surface tension is also responsible for the fact that small insects can \u201cwalk\u201d on water. Because of surface tension, it takes energy to break the surface of a liquid, and if an object (such as an insect) is light enough, there is not enough force due to gravity for the object to break through the surface, so the object stays on top of the water (Figure 10.9 \"Walking on Water\"). Carefully done, this phenomenon can also be illustrated with a thin razor blade or a paper clip.\r\n\r\n[caption id=\"attachment_591\" align=\"aligncenter\" width=\"400\"]\"Small Figure 10.9 \"Walking on Water.\" Small insects can actually walk on top of water because of surface tension effects.[\/caption]\r\n\r\nThe fact that small droplets of water bead up on surfaces does not mean that water \u2014 or any other liquid \u2014 does not interact with other substances. Sometimes the attraction can be very strong. Adhesion<\/strong> is the tendency of a substance to interact with other substances because of intermolecular forces, while cohesion<\/strong>\u00a0is the tendency of a substance to interact with itself. If cohesive forces within a liquid are stronger than adhesive forces between a liquid and another substance, then the liquid tends to keep to itself; it will bead up. However, if adhesive forces between a liquid and another substance are stronger than cohesive forces, then the liquid will spread out over the other substance, trying to maximize the interface between the other substance and the liquid. We say that the liquid wets<\/em> the other substance.\r\n\r\nAdhesion and cohesion are important for other phenomena as well. In particular, if adhesive forces are strong, then when a liquid is introduced to a small-diameter tube of another substance, the liquid moves up or down in the tube, as if ignoring gravity. Because tiny tubes are called capillaries, this phenomenon is called capillary action<\/strong>. For example, one type of capillary action \u2014 capillary rise <\/em>\u2014 is seen when water or water-based liquids rise up in thin glass tubes (like the capillaries sometimes used in blood tests), forming an upwardly curved surface called a meniscus<\/strong>. Capillary action is also responsible for the \u201cwicking\u201d effect that towels and sponges use to dry wet objects; the matting of fibres forms tiny capillaries that have good adhesion with water. Cotton is a good material for this; polyester and other synthetic fabrics do not display similar capillary action, which is why you seldom find rayon bath towels. A similar effect is observed with liquid fuels or melted wax and their wicks. Capillary action is thought to be at least partially responsible for transporting water from the roots to the tops of trees, even tall ones.\r\n\r\nOn the other hand, some liquids have stronger cohesive forces than adhesive forces. In this case, in the presence of a capillary, the liquid is forced down from its surface; this is an example of a type of capillary action called capillary depression<\/em>. In this case, the meniscus curves downward. Mercury has very strong cohesive forces; when a capillary is placed in a pool of mercury, the surface of the mercury liquid is depressed (Figure 10.10 \"Capillary Action\").\r\n\r\n[caption id=\"attachment_5449\" align=\"aligncenter\" width=\"600\"]\"\" Figure 10.10 \"Capillary Action.\" (a) Capillary rise is seen when adhesion is strong, such as with water in a thin glass tube. (b) Capillary depression is seen when cohesive forces are stronger than adhesive forces, such as with mercury and thin glass tubes.[\/caption]\r\n\r\n
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        Chemistry Is Everywhere: Waxing a Car<\/h1>\r\nResponsible car owners are encouraged to wax their cars regularly. In addition to making the car look nicer, it also helps protect the surface, especially if the surface is metal. Why?\r\n\r\nThe answer has to do with cohesion and adhesion (and, to a lesser extent, rust). Water is an important factor in the rusting of iron, sometimes used extensively in outer car bodies. Keeping water away from the metal is one way to minimize rusting. A coat of paint helps with this. However, dirty or scratched paint can attract water, and adhesive forces will allow the water to wet the surface, maximizing its contact with the metal and promoting rust.\r\n\r\nWax is composed of long hydrocarbon molecules that do not interact well with water. (Hydrocarbons are compounds with C and H atoms; for more information on hydrocarbons, see Chapter 16 \"Organic Chemistry\"<\/a>.) That is, a thin layer of wax will not be wetted by water. A freshly waxed car has low adhesive forces with water, so water beads up on the surface, as a consequence of its cohesion and surface tension. This minimizes the contact between water and metal, thus minimizing rust.\r\n\r\n[caption id=\"attachment_593\" align=\"aligncenter\" width=\"400\"]\"Droplets Figure 10.11 Droplets of water on a freshly waxed car do not wet the car well because of low adhesion between water and the waxed surface. This helps protect the car from rust.[\/caption]\r\n\r\n<\/div>\r\n
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        Key Takeaways<\/p>\r\n\r\n<\/header>\r\n

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