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Topic B.2 Reference: pages 559 - 569 What IS Thermodynamics? A branch of physics that studies the effects of work, heat, and energy on a system. The study of the conditions under which thermal energy can be transferred through performing mechanical work Thermodynamics only focuses on large-scale observations (in other words, we’re no longer focusing on the behavior of individual molecules in a system, but, rather, the entire sample) Review… What is WORK? A force acting through a distance to transfer energy What are the Macroscopic properties that we use when describing a thermal system of gas? Macroscopic Properties: Pressure, Volume and Temperature—all used to determine the amount of work that is/can be done by or to a sample of gas. HOW could we do work on an enclosed sample of gas? Systems The complete set of objects being considered in a particular scenario/problem Open System Mass is free to enter and/or leave the system Closed System Mass is not free to enter and/or leave the system. The quantity of the gas will remain constant Isolated System No energy in any form can enter or leave the system No mass can enter or leave the system State of a System The State of a system is known when particular quantifiable characteristics of the system are known, such as the following: Pressure Volume Temperature Internal Energy These are each a State Function: a characteristic of the system. Note: If two gases, originally in different (thermodynamic) states, are brought to the same state, the gases will have the same internal energy—no matter how they got there. Non-state functions Thermal Energy and Work Doing work, or adding or removing thermal energy Related to a CHANGE in the state, not in the state itself A gas does not “contain” thermal energy—it can transfer it when it changes state A gas does not “contain” work—it has work done to it when compressed, or work done by it when expanded Thermodynamic Processes Thermodynamic Processes are any processes that will result in the change of the state of a system Heating a gas Compressing the gas (doing work TO the gas) Expansion of the gas (work done BY the gas) Internal Energy: Reminders/Review Internal Energy: The sum of the total kinetic energy of the molecules in a sample of a gas and the potential energy associated with the intermolecular forces with that gas. Ideal Gases: assume that the intermolecular forces are nonexistent, so potential energy = 0 Therefore the internal energy is solely related to the kinetic energy (which is random…each molecule is likely different) Average Kinetic Energy: 𝐸𝐾 = 32𝑘𝑇 Internal Energy Internal energy of a fixed quantity of a gas (constant number of moles) will only depend on the temperature. It does NOT depend on volume or pressure Free-Expansion: when a gas is allowed to expand in a way that is not constricted—both the volume an pressure change in such a way that the temperature will remain constant (in an ideal gas) Thus—the internal energy is constant for a given temperature of ideal gas. Work Done by/to a Gas Imagine a Piston—cross sectional area A Change the position of the piston by applying a force to expand or compress the gas Volume changes W = P·ΔV PV diagrams PV Diagrams Total work done by the gas as it expands (or to the gas as it’s compressed) = area under the curve Closed loop? Total (net) work done to/by the system = enclosed area Thermodynamic Processes Review: What do we call the following processes: When the pressure remains constant, but volume and temperature change When the volume remains constant, but the pressure and temperature change When the temperature remains constant, but the pressure and volume change Isobaric Processes Those processes in which the pressure of the system remains constant while the volume and temperature change Results in a horizontal line on a PV diagram (Isobar) Isochoric Processes Those processes in which the volume remains constant while the pressure and temperature change Results in a vertical line on the PV diagram (an Isochore) No work is done during an isochoric process Isothermal Process Those processes in which the temperature remains constant (and, as a result, the internal energy) The pressure and volume will each change Adiabatic Process Pressure, Volume, and Temperature all change in a way so that no thermal energy (heat) is transferred between the system and the surroundings Happens in a very well-insulated container Happens very quickly Energy does not have time to leave the system, so the result is that the temperature will change (because internal energy changes) Adiabatic Processes Adiabatic Expansion: Pressure decreases Volume increases Temperature decreases Adiabatic Compression: Pressure increases Volume decreases Temperature increases Energy Transfers Energy is conserved If work is done to a system, energy is transferred into the system in some form If work is done by a system, energy is transferred away from the system in some form Forms of energy: Internal Energy (related to the temperature) Thermal energy st 1 Law of Thermodynamics 𝑸 = ∆𝑼 + 𝑾 Q = Thermal energy / J When (+) , energy is transferred into the system Surroundings are at a higher temperature than the system When (-) , energy is transferred into the surroundings System is at a higher temperature than the surroundings st 1 Law of Thermodynamics 𝑸 = ∆𝑼 + 𝑾 DU = Change in Internal Energy When + , represents the increase in internal energy When - , represents the decrease in internal energy st 1 Law of Thermodynamics 𝑸 = ∆𝑼 + 𝑾 W Work done When + , represents the work done BY the system as the gas expands When - , represents the work done TO the system System causes the gas to compress. Practice Problem An ideal gas is held in a cylinder by a moveable piston and energy is supplied to the gas such that the gas expands at a constant pressure of 1.50 x 105 Pa. The initial volume of the cylinder is 0.040 m3 and its final volume is 0.12 m3. The total energy supplied to the gas during the process is 7.5 x 103 J. State and explain the type of change that the gas undergoes Determine the work done by the gas Calculate the change in internal energy of the gas.