Aubrey High School AP Chemistry Name ___________________________________ Period ___ Date ___/___/___ 6 Thermodynamics 6.1 Lesson – Enthalpy Change in Internal Energy (∆Eint) It’s important to define the system − that at which we’re looking, usually a container or a physical or chemical process − and the surroundings – the rest of the universe, so we can study the movement of energy between them. Open System Movement of Matter between System and Surroundings Movement of Energy between System and Surroundings Closed System Isolated System The internal energy (Eint) of a system is the sum of all of the kinetic energy (which contributes to the temperature) and potential energy (from attractions between particles). The First Law of Thermodynamics states that in an isolated system (one in which no matter or energy can be exchanged), the internal energy of the system is conserved (∆Eint = 0): energy can be converted from one form or another (such as from kinetic energy to potential energy), but the total energy cannot increase or decrease. However, no system is truly isolated, so the internal energy of a closed system can change in two ways: (1) heat flow or (2) work. ∆Eint = q + w Heat (q) is the flow of thermal energy between the system and the surroundings from the object of higher temperature to that of lower temperature. q = m·c·∆T Work (w) can be measured by the energy from the expansion or compression of a gas. w = −P·∆V Example 1: A 20.0 g sample of Ar (g) in a cylinder with a piston at 30°C. Heat flows into the cylinder and increases the temperature to 40°C. The cylinder expands against a constant pressure of 95.5 kPa from 21.5 L to 23.5 L. By how much has the internal energy of the system changed? Ar has a specific heat of 0.52 J/g·°C. (1 J = 1 L·kPa). Ideas about Heat (q) Example 2: A student dissolves 10.0 g of NaOH in 100.0 mL of distilled water, and notices the temperature of the mixture increase from 25.0°C to 51.6°C. (a) The student states: The process of dissolving NaOH is endothermic, because the temperature increases (i.e. ∆T > 0) so q > 0. Do you agree or disagree? Why? Use system, surroundings, heat, endothermic, and exothermic in your explanation. (b) Explain in terms of molecular motion what is happening when the temperature of the water is increasing. (c) Describe (pictorially) the substances before (NaOH (s) and H2O (ℓ)) and after the dissolution (NaOH (aq)). Identify the inter-particle forces involved in the substances before and after the dissolution. Do the substances before the dissolution have less or more potential energy than those after the dissolution? BEFORE: AFTER: (d) Describe the process of breaking and forming inter-particle forces/attractions in the dissolution of NaOH. Draw a potential energy diagram for each step of the process. Then explain why the temperature lowers when dissolving a different salt, NH4Cl (s). (e) Calculate the heat flow (q) for this process. The specific heat of water is 4.18 J/g·°C. (f) Calculate the ∆Hdiss for this process: NaOH (s) → NaOH (aq) Enthalpy of Reaction (∆Hrxn) Example 3: Consider the reaction: 2 SO2 (g) + O2 (g) → 2 SO3 (g) (a) Experimental Approach to Determining ∆Hrxn A 9.71 g sample of SO2 (g) reacts with excess O2 releasing 15.0 kJ of energy. Calculate ∆Hrxn. (b) Products – Reactants Approach Using the ∆Hrxn from part (a), determine the value of ∆Hf for SO2 (g). ∆Hf for SO3 (g) is −396 kJ/mol. (c) Hess’s Law Calculate the value of ∆Hrxn using the following reactions. Compare the result with that found in part (a). 2 H2S + 3 O2 → 2 H2O + 2 SO2 ∆H1 = −1124 kJ/mol (1) (2) H2O + SO3 → H2SO4 ∆H2 = −132 kJ/mol (3) H2S + 2 O2 → H2SO4 ∆H3 = −793 kJ/mol (d) Bond Energy Approach Using the following structures and bond energies, calculate the ∆Hrxn. Compare the result with that found in part (a) (and explain any difference). Lewis Structures: SO2 Bond Energies S=O O=O Draw the graph of the potential energy vs. inter-nuclear distance for both the S=O and O=O bonds to show why the bond energy for S=O is greater than that of O=O. SO3 522 kJ/mol 495 kJ/mol
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