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LECTURE 10 PHASES, & Lecture Instructor: Kazumi Tolich Lecture 10

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¨ Reading chapter 13-5 to 13-6 & 14-3. ¤ equilibrium ¤ Evaporation ¤ Latent heats n Latent heat of fusion n Latent heat of n Latent heat of sublimation Phase equilibrium

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¨ If a substance has two or more phases that coexist in a steady and stable fashion, the substance is in phase equilibrium.

¨ The of the when equilibrium is reached is called equilibrium pressure. Vapor-pressure curve

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¨ A plot of the equilibrium versus is called vapor-pressure curve.

¨ A boils at the temperature at which its vapor pressure equals the external pressure. Pressure cookers

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¨ The pressure inside the cooker is higher than , so the boils at the higher temperature.

¨ Food cooks faster at the higher temperature.

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¨ A fusion curve indicates where the and liquid phases are in equilibrium.

¨ A sublimation curve indicates where the solid and gas phases are in equilibrium.

¨ A plot showing a vapor-pressure curve, a fusion curve, and a sublimation curve is called a phase diagram.

¨ The vapor-pressure curve comes to an end at the critical point. Beyond the critical point, there is no distinction between liquid and gas.

¨ At , all three phases, solid, liquid, and gas, are in equilibrium.

¤ In water, the triple point occur at T = 273.16 K and P = 611.2 Pa. Slope of the fusion line

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¨ In most substances, the fusion line has a positive slope.

¨ As the pressure increases, the temperature of the substance also increases because a solid is denser than the corresponding liquid.

¨ In water, the slope is negative because ice is less dense.

Typical substance Water Example: 1

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¨ The phase diagram for water is shown.

a) What is the temperature T1?

b) What is the temperature T2? c) What happens to the melting/ temperature if atmospheric pressure is decreased?

d) What happens to the / temperature if atmospheric pressure is increased? Evaporation

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¨ If you leave a cup of water out at room temperature, the water eventually evaporates.

¨ The temperature of the water reflects the average of the water .

¨ The most energetic molecules have enough energy to break loose from the molecular bonds at the surface of the water.

¨ As these highest-energy molecules leave the water, the average energy of those left behind decreases.

¨ Evaporation is a cooling process. Demo: 1

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¨ Freezing water by evaporation ¤ When the pressure is lowered, water boils at a lower temperature. ¤ Evaporation of water lowers the temperature of water itself. Evaporating 11

¨ The average kinetic energy of the molecules is proportional to temperature. H2 He ¨ For the temperature of Earth’s atmosphere, O2 most of N2 and O2 are moving at speed much less than the escape speed.

¨ Having higher speed, most of H2 and He have escaped.

¨ The escape speed at the surface of the moon is 2.3 km/s, so all gas molecules/ escaped, and the moon does not have atmosphere. Latent heats

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¨ When two phases coexist, the temperature remains the same even if a small amount of heat is added.

¨ Instead of raising the temperature, the heat goes into changing the phase of the material, breaking the intermolecular attractions. Latent heats: 2

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¨ The energy required to convert a substance of mass m from one phase to another is given by Q = mL where L is the coefficient of latent heat.

¤ The latent heat to melt (or fuse) is the latent heat of fusion, Lf.

¤ The latent heat to convert a liquid to a gas is the latent heat of vaporization, Lv.

¤ The latent heat to convert a solid to a gas is the latent heat of sublimation, Ls.

Demo: 2

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¨ CO2 sublimation

¤ Demonstration of sublimation of CO2 Example: 2

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¨ A of Q = 9.5 × 105 J is required to convert a block of ice at Ti = -12 °C to Tf = 12 °C. What was the mass of the block of ice? Clicker question: 1

16 Example: 3

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¨ can cause more serious burns than water at the same temperature. Flesh becomes badly damaged when its temperature reaches 50.0 °C.

a) Calculate the heat released as

m = 12.5 g of liquid water at Ti = 100 °C is cooled to Tf = 50.0 °C. b) Calculate the heat released as

m = 12.5 g of steam at Ti = 100 °C is condensed and cooled to Tf = 50.0 °C. c) Calculate the mass of flesh that can be

heated from T’i = 37.0 °C (normal body temperature) to T’f = 50.0 °C. The average specific heat of flesh is cflesh = 3500 J/kgŸK. Clicker question: 2

18 Water protects buds from cold weather

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¨ When temperature falls a few degrees below 0 °C, fruit crop is in danger of being ruined.

¨ To protect the buds, farmers spray the trees with water.

¨ Water has large latent heat of fusion.

¨ Before the buds can freeze, the water must be cooled to 0 °C and then freeze.

¨ In this process, the water gives up heat and keeps the temperature of the buds from going below 0 °C.

¨ The layer of ice over the buds acts like insulation because ice is not a good conductor of heat.