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Heat and Thermodynamics
1.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 1 Rapid Learning Center Chemistry :: Biology :: Physics :: Math Rapid Learning Center Presents …p g Teach Yourself AP Physics in 24 Hours 1/67 *AP is a registered trademark of the College Board, which does not endorse, nor is affiliated in any way with the Rapid Learning courses. H t d Th d iHeat and Thermodynamics Physics Rapid Learning Series Rapid Learning Center www.RapidLearningCenter.com/ © Rapid Learning Inc. All rights reserved. Wayne Huang, Ph.D. Keith Duda, M.Ed. Peddi Prasad, Ph.D. Gary Zhou, Ph.D. Michelle Wedemeyer, Ph.D. Sarah Hedges, Ph.D.
2.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 2 Learning Objectives Temperature: Understand the definition of temperature. By completing this tutorial, you will learn: Energy in Thermal Processes. Understand the relationship between heat and internal energy. Thermal Processes in your world. Global warming and greenhouse gasses. 3/67 Laws of Thermodynamics. Apply the laws of thermodynamics to real life problems such as engines and human metabolism. Concept Map Physics Studies Previous content New content Thermodynamics The field of Matter and EnergyMatter and Energy Heat Energy One type of energy is 2nd Law1st Law Expansion Thermal Expansion 4/67 17 : 3/68 Heated objectsHeated objects expand Energy is destroyed Energy is neither created nor destroyed Entropy increases Entropy always increases States thatStates that States that
3.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 3 ThermodynamicsThermodynamics and Thermal Expansion Thermometers and Temperature Scales. Thermal expansion of Solids and Liquids 5/67 Thermal expansion of Solids and Liquids Thermodynamics and Temperature How does temperature affect materials and how is this used to measure temperature? Linear expansion Volume expansion The physics of thermostats The physics of 6/67 thermometers
4.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 4 Definition - Thermodynamics Thermodynamics - The branch of physics that deals with conversionsphysics that deals with conversions between heat energy and other forms of energy. 7/67 Thermal Expansion As solids and liquids are heated, they expand because their molecules gain kinetic energy and move around more. Expansions of solids can be predicted using the linear expansion equation. Expansions of liquids can be predicted using the volume expansion equation. 8/67 p q The ticking noises heard after a hot car is shut down are due the shape changes of engine parts as they cool.
5.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 5 Linear Expansion Equation The linear expansion equation is of the form: Where: L = length of object T = temperature ∆TαL∆L ××= 9/67 p α = coefficient of linear expansion [units = per degree] ∆ = Greek letter “delta”, change in. Volume Expansion Equation Similarly, the volume expansion equation is of the form: ∆TβV∆V ××= Where: V = volume of object T = temperature ∆TβV∆V ××= 10/67 ß = coefficient of volume expansion [units = per degree] ∆ = Greek letter “delta”, change in.
6.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 6 Expansion Coefficients Note the units of the expansion coefficients: 1∆L α ×= 1∆V β ×= The linear and volume expansion coefficients are Thus, length and volume cancel. Both expansion coefficients have units of “per degree” ∆TL α × ∆TV β × 11/67 The linear and volume expansion coefficients are related to each other by the following relationship: Typical values for expansion coefficients may be found in your physics textbook. α3β ×= Sample Problem: Thermal Expansion Question: How much will the volume of a 2 cm3 aluminum cube change if the temperature changes from 12°C to 32°C? The linear expansion coefficient, α, of aluminum is 23x10-6/°C. S l tiSolution: Step 1: Use the volume expansion equation. ∆V = Vß * ∆T Step 2: Calculate ∆T. ∆T = Tfinal –Tinitial = 32°C – 12°C = 20°C St 3 C l l t ß 12/67 Step 3: Calculate ß. ß = 3α = 3 * 23 x10-6/°C = 69 x 10-6/°C Step 4: Plug in the values. ∆V = Vß * ∆T = (2cm3) * (69x10-6/°C) * (20°C) Answer: ∆V = 2.76x10-3 cm3
7.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 7 Note - Units and Temperature Change 13/67 Thermostats - 1 Thermostats are designed to measure temperature by applying the principle of linear expansion. A thermostat uses two fused strips of metal, each with a different linear expansion coefficient. As the strip heats up one strip lengthens faster so the strips 14/67 bend away from the longer strip. Typically the bent strips will make contact with a circuit.
8.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 8 Thermostats - 2 Imagine a thermostat made up of two metal strips as shown below. The yellow strip has a larger linear expansion coefficient. Heat 15/67 Heat The strip bends towards the side with the lower linear expansion coefficient. Thermometers Thermometers are designed to measure temperature by applying the principle of thermal expansion. Most home thermometers use mercury or alcohol inside a narrow glass tube. As the temperature rises, both the glass and liquid expand. The liquid has a higher volume 16/67 The liquid has a higher volume expansion coefficient than the glass tube so it rises within the tube to tell you the temperature.
9.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 9 Thermal Expansion: Stop-And-Think Question: Why would engineers need to take thermal expansion into account in the design of bridges? On hot days, the metal supports of a bridge will expand and buckle if the bridge is not designed to expand. Similarly, the bridge will crack as the supports shrink on a cold day. 17/67 Energy in Thermal Processes Heat and Internal Energy Specific Heat 18/67 Specific Heat Calorimetry Latent Heat and Phase Change Energy Transfer Global Warming and Greenhouse Gasses
10.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 10 System vs. Surroundings Calculations of heat and internal energy are based on the definition of a system and its surroundings. System - The system refers to the object being studied. Surroundings - 19/67 g Everything not included in the system. Example - System v. Surroundings Example: a beaker The system refers to the contents of the beaker. Th di f 20/67 The surroundings refer to everything else.
11.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 11 Heat and Internal Energy Equation Internal energy of a system is defined as: 1) The ability to do work on an object. 2) The ability to transfer heat to an object. U = q + w Heat Heat energy of the system 21/67 q Internal Energy Work System internal energy Work done on the system or energy available for the system to do work. Definition - Energy Units Calorie (cal) - Heat is measured in calories. A calorie is the amount of heat required to heat 1 gram of water 1°C. Joule (J) - Energy is measured in Joules. One calorie (cal) is equal to 4 18J 22/67 4.18J. 4.18 J = 1 cal
12.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 12 Definition - State Function State Function - n. A state function is a quantity of the object that isa quantity of the object that is dependent on the current state. A state function is independent of the path taken to reach the current state. 23/67 Temperature, kinetic energy, and potential energy are all state functions. Temperature is a State Function Temperature is an example of a state function. Your coffee can be 40°C whether you heated it in the microwave or on the stove. 24/67 40°C
13.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 13 Note: the Food Calorie 25/67 Definition - Specific Heat Specific Heat (CP) - n. Specific heatp ( P) p is a material property that defines the quantity of heat, q, required to raise 1g of a specific material 1°C. 26/67 units of cp = [cal/gram*K]
14.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 14 Specific Heat Equation T T The specific heat may be used as follows: Q = CPm * ∆T Specific Heat Change in Temperature Tfinal - Tinitial (K) or (°C) Proportionality Constant J/g*K or cal/g*K 27/67 P Heat Total Heat Energy (J) Mass Mass of Object (g) Interpretation of Specific Heat What are the practical implications of specific heat? High Specific Heat Low Specific Heat Large amount of energy to change temperature Small amount of energy can change temperature Heats up slowly Cools down slowly Small temperature changes with condition changes e g Water Cast iron Heats up quickly Cools down quickly Quickly readjusts to new conditions e g Air aluminum foil 28/67 e.g. Water, Cast-iron e.g. Air, aluminum foil A pool takes a long time to warm up and remains fairly warm over night. The air warms quickly on a sunny day, but cools quickly at night A cast-iron pan stays hot for a long time after removing from oven. Aluminum foil can be grabbed by your hand from a hot oven because it cools so quickly
15.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 15 Specific Heat and Heat Capacity Thus, if the specific heat and the mass of any object are known, then the amount of heat need to raise the temperature by any given amount may be calculated. The heat capacity C of an object may be determined from its specific heat CP and its mass m as follows: CmC × 29/67 C = heat capacity CP = specific heat m = mass of object pCmC ×= Definition - Heat Capacity Heat Capacity (C) - The amount of heat Q required to raise the temperature of an object by ∆T is given by: Q = C * ∆T Heat Capacity Proportionality Constant J/K or cal/K object by ∆T is given by: 30/67 Q = C * ∆T Heat Change in Temperature Tfinal - Tinitial (K) or (°C) Total Heat Energy (J)
16.
AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 16 Definition - Enthalpy (H) Enthalpy of Reaction (H) - The enthalpy of a reaction is the heat energy (J) gained or lost during a reaction. Enthalpy is a state function.during a reaction. Enthalpy is a state function. Reaction Bonds of reactants broken. Bonds of products formed. Bonds of reactants have hi h th Bonds of products have higher energy than 31/67 higher energy than bonds of products. higher energy than bonds of reactants. Exothermic Endothermic Heat given off by system Heat absorbed by system Endothermic vs. Exothermic Exothermic - If the system looses net heat during a reaction, the reaction isg , exothermic. Endothermic - If the system gains net ∆Hsystem = Hfinal – Hinitial < 0 32/67 y g heat energy during a reaction, the reaction is endothermic. ∆Hsystem = Hfinal – Hinitial > 0
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 17 Definition - Calorimetry Calorimetry. n. Calorimetry is aCalorimetry is a laboratory technique used to determine the amount of heat Q taken up or given off 33/67 by a reaction. Procedure - Calorimetry A small beaker is immersed in an insulated1 How to determine the heat of a reaction using calorimetry. beaker filled with a known amount of water. The initial temperature of the water is noted. A known amount of the reactants are placed in the small reaction beaker. The temperature of the water is recorded at 1 2 3 4 34/67 regular intervals as the reaction proceeds. The change is temperature is plotted versus time. 4 5 6 The heat given off by the reaction is calculated from the total change in temperature of the water.
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 18 Example - Calorimetry (1) Large, insulated beaker (2) Water initial(2) Water, initial temperature Tinitial (3) Reaction beaker (4) Initiate reaction 35/67 (5) Flow of heat energy to water (6) Measure final water temperature, Tfinal (7) Calculate ∆H from ∆Twater and the specific heat of water, CP. Endothermic vs. Exothermic Reactions Endothermic Exothermic Heat moves from Heat moves from system surroundings to system Internal energy of system increases KEAVE of system molecules increases Internal energy of system decreases KEAVE of the system decreases to surroundings. 36/67 Temperature of the system increases Bonds of reaction products have greater energy than bonds of reactants Temperature of the system decreases. Chemical bonds of reactants have greater energy than bonds of products.
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 19 Stop and Think- Calorimetry Question: If the temperature of the water in a l i t i t i i th ticalorimetry experiment rises, is the reaction endothermic or exothermic? Answer: The reaction is exothermic because heat energy is moving from the system (the reaction) to 37/67 energy is moving from the system (the reaction) to the surroundings (the water). Latent Heat and Phase Change A rise in temperature Internal energy increases When a solid is heated it undergoes the following: Internal energy increases Molecules oscillate more rapidly A phase change from solid to liquid Molecules oscillate so rapidly they loose their crystalline form There is no increase in temperature during the transition Another rise in temperature 38/67 Another rise in temperature A phase change from liquid to gas Molecules oscillate so rapidly they escape the intermolecular forces that bind them together and enter the gas phase There is no increase in temperature during the transition.
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 20 Heats of Fusion and Vaporization The amount of heat Qfus needed to melt m grams of a substance is given by the following equation: fusfus Lm∆Q ×= Qfus = heat energy = [calories] m = mass = [grams] Lfus = Heat of Fusion = [calories/gram] The amount of heat Qvap needed to vaporize m grams of a substance is given by the following equation: fusfus Lm∆Q × 39/67 Qvap = heat = [calories] m = mass = [grams] Lvap = Heat of Vaporization = [calories/gram] of a substance is given by the following equation: vapvap Lm∆Q ×= Latent Heat and Phase Change Gas Temperatureof Substance Phase Liquid Phase Solid Tboil Tmelt 40/67 Increase in Heat Energy, ∆Q Solid Phase Qmelt Qboil
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 21 Example - Heats of Transformation Question: How much heat energy is required for 10 grams of ice at 0°C to transition to liquid? To evaporate? The heat of fusion for water is 333 KJ/kg. The heat of vaporization is 2256 KJ/kg. Solution:Solution: 1) Calculate the heat energy required to melt 10 grams (0.01Kg) of ice. Qfus = Lfus * m = 333 KJ/kg * 0.01 Kg = 3.33 KJ 2) Calculate the heat energy needed to raised the temperature of the water from 0°C to 100°C. Q = 0.00418 KJ/g*°C * 10.0 g * (100-0)°C = 4.18 kJ 41/67 3) Calculate the heat energy required to vaporize 10g of water. Qvap = Lvap * m = 2256 KJ/kg * 0.01Kg = 22.56 KJ 4) The total heat required is the sum of 1-3. Qtot = 3.33 KJ + 4.18 KJ + 22.56 KJ = 30.07 KJ Answer: Qtot = 30.07 KJ Stop-and-think- Sweating Question: Why is sweating an effective cooling mechanism? 42/67 Answer: As sweat evaporates from your skin it transitions from the liquid to the gas phase. This phase transition requires a transfer of heat energy from the skin to the liquid, cooling the skin.
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 22 Global Warming & Greenhouse Gases 1) Heat energy radiates from the sun to the earth 2) Some of the heat energy is reflected off greenhouse gasesreflected off greenhouse gases in the earth’s atmosphere. 3) Some of the heat energy is reflected of the earth’s surface. 4) Some of the energy reflected off the surface is trapped by greenhouse gases in the 43/67 atmosphere. 5) As the concentration of greenhouse gases is increased due to emissions from cars and factories, the temperature of the earth rises. The Laws of Thermodynamics The Zeroth Law of Thermodynamics Work in Thermodynamic Processes 44/67 Work in Thermodynamic Processes The First Law of Thermodynamics Heat, Engines, and the Second Law of Thermodynamics Entropy Human Metabolism
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 23 Heat Energy and the Laws of Thermodynamics The Zeroth Law of Thermodynamics states that objects in thermal ilib i t th The laws of thermodynamics govern energy exchanges: equilibrium are at the same temperature. The internal energy of a system is the sum of the heat energy of the system and the work done on or by the system. The 1st Law of Thermodynamics states that energy can change state but cannot 45/67 gy g be created or destroyed. The 2nd Law of Thermodynamics states that the total entropy, or disorder, of the universe can increase or stay the same but never decrease. The universe tends towards disorder. Definition: Thermal Equilibrium Thermal Equilibrium - Two objects are thermal equilibrium are at the sameq temperature. That is, when put in contact they remain at the same temperature and no longer exchange net heat energy. A and B areIf A is placed inThe temperature 46/67 A and B are said to be in thermal equilibrium. p contact with B, they both remain at 10C°. The temperature of A is 10C° and the temperature of B is 10C° Note that if objects are in thermal equilibrium, their molecules also have the same average kinetic energy
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 24 Zeroth Law of Thermodynamics Zeroth Law - If object A is in thermal equilibrium with object B and object C, then objects B and C are also in thermalthen objects B and C are also in thermal equilibrium. A 10 degrees Celsius 47/67 B C 10 degrees Celsius 10 degrees Celsius Note that if B and C are in thermal equilibrium with A, then they must also be at 10 degrees Celsius. Work in Thermodynamics As mentioned before: U = q +U = q + w U = system internal energy q = heat energy w = work done on or by the system 48/67
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 25 Pressure-Volume Work For constant pressure: ∆W = -P * ∆V ∆W = work done on or by the system P = pressure ∆V = volume change of the system One common type of application of this equation is in calculating pressure-volume work done by 49/67 engines. Applied Pressure-Volume Work If the system expands, work is done by the system on the surroundings. The internal energy of the systeminternal energy of the system decreases. If the system contracts, work is done 50/67 by the surroundings on the system. The internal energy of the system increases.
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 26 The First Law of Thermodynamics Energy in a reaction may be changed from one form to another but it is neither t d d t d ti fcreated nor destroyed – conservation of energy. 51/67 Application of The 1st Law This implies that: Q Q ∆U = ∆q + ∆w Change in Heat Energy W k d t b Qinitial -Qfinal 52/67 Change in System Internal Energy Work done to or by the system Ufinal - Uinitial Win -Wout
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 27 Work and the 1st Law There are 4 special applications of the 1st Law: 1) Adiabatic: Q = 0, ∆U = -W 2) Constant-volume: W = 0, ∆U = Q 3) Cyclical: ∆U = 0, Q = -W 53/67 4) Free expansion processes: ∆U = Q = W Adiabatic Work An example of adiabatic work is a closed system with a piston. If pressure is applied rapidly to depress the piston, the volume of the system will decrease. Work W is done on the system by the surroundings, but there is ∆V ≥ 0 Q = 0, ∆U = -W = -P*∆V is done on the system by the surroundings, but there is no change in heat Q so the change in internal energy ∆U is equal to –W. W 54/67 W Vinitial Vfinal
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 28 Constant-Volume Work An example of constant-volume work is heating a sealed cylinder. There is no volume change so the change in internal energy is equal to the change in heat energyenergy. Tinitial Tfinal 55/67 ∆V = 0 so W = 0 ∆T ≥ 0 so Q ≥ 0 ∆U = Q Cyclical Work and Engines In an engine, heat is used to increase pressure leading to an increase in volume. The change in volume does work on the surroundings. The work energy is transferred back from the surroundings to compress the cylinder back to its original size and the cycle repeatsand the cycle repeats. ∆U = 0 Q W 56/67 Q = -W
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 29 Free Expansion Work Connecting a pressurized system to a vacuum is an example of free-expansion work. The gas from the pressurized system will immediately and irreversibly expand to fill the vacuum The process occurs rapidlyexpand to fill the vacuum. The process occurs rapidly, but unlike adiabatic work the process is irreversible. ∆U = Q = W = 0 Heating an open beaker may be considered free- i k Th t th t t f th 57/67 expansion work. The system, the contents of the beaker, are open to the surroundings so there can be no volume changes or heat exchanges. Energy Calculations: Example Question: If the volume of a sealed balloon increases from 10mL to 100mL when heated and then shrinks back to 10mL as it cools, what f tapplication of the 1st Law is this? Constant-volume Adiabatic 58/67 Cyclical
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 30 Energy Calculations: Answer Question: If the volume of a sealed balloon increases from 10mL to 100mL when heated and then shrinks back to 10mL as it cools, what f tapplication of the 1st Law is this? Constant-volume Adiabatic 59/67 Cyclical Definition - Entropy Entropy (S) - n. Entropy is a measure of the disorder of a system or its surroundings.surroundings. 60/67 A landfill possesses lots of entropy!
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 31 The 2nd Law of Thermodynamics The 2nd Law of Thermodynamics states that the total entropy of the universe can never decrease, it can only increase or stay the same. ∆Stotal ≥ 0 Note that the entropy of the system may decrease, so long as the entropy of the s rro ndings increases b an eq al or greater 61/67 surroundings increases by an equal or greater amount. Thus, ∆Ssys + ∆Ssur ≥ 0 Relative Entropies Low entropy states are more organized than high entropy states. Lower Entropy Higher Entropy Your clean bedroom Your room after finals Solids Liquids 62/67 Liquids Salt tablets in water Gases Dissolved salt in water
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 32 Definition - Engine Efficiency In a real combustion engine such as your car, some of the work energy is lost to the surroundings as heat rather than transferred to pressure-volume work which moves a piston. The efficiency of an engine is the ratio of the heat energy put in (for example by combustion) to the work output by the engine (such as movement of the wheels of a car). ε = Wout / Qin 63/67 If the efficiency of an engine is 0.7, the 30% of the heat from combustion is lost as heat to the surroundings. In the real world, this would be a very efficient engine!!! Entropy and Human Metabolism Question: Metabolic processes in the body, such as the building of proteins and DNA, lead to increased order. How does this not violate the 2nd Law? Answer: Although the building of structural proteins in the body lead to increased order in the system, which is the body, they lead to increased disorder in the surroundings through loss of heat. 64/67 surroundings through loss of heat. Metabolic processes are usually linked to a catabolic process such as the combustion of glucose or the flow of ions down a concentration gradient.
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 33 Entropy: Stop-and-Think Question Question: When an ice cube melts, does system entropy increase, decrease, or remain the same? Pick the best answerPick the best answer. A. Remain the same because there is no reaction, only a state change. B. Increase because the molecules are changing 65/67 g g from an ordered crystalline state to a disordered liquid state. C. Decrease because heat is absorbed to melt the ice. Entropy: Stop-and-Think Answer Question: When an ice cube melts, does system entropy increase, decrease, or remain the same? Pick the best answerPick the best answer. A. Remains the same because there is no reaction, only a state change. B. Increases because the molecules are changing 66/67 g g from an ordered crystalline state to a disordered liquid state. C. Decreases because heat is absorbed to melt the ice.
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 34 Entropy is aEntropy is a Expansion coefficients measure how Expansion coefficients measure how The 2nd Law states that net entrop can The 2nd Law states that net entrop can Learning Summary Heat energy mayHeat energy may measure of disorder. measure of disorder. measure how much objects expand when heated. measure how much objects expand when heated. entropy can never decrease. entropy can never decrease. The 1st LawThe 1st Law 67/67 Heat energy may be gained or lost to the surroundings during work. Heat energy may be gained or lost to the surroundings during work. The 1 Law states that energy is never created or destroyed. The 1 Law states that energy is never created or destroyed. Congratulations Y h f ll l t dYou have successfully completed the tutorial Heat and Thermodynamics 68/67 Rapid Learning Center
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AP Physics Rapid
Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 35 Rapid Learning Center Wh t’ N t Chemistry :: Biology :: Physics :: Math What’s Next … Step 1: Concepts – Core Tutorial (Just Completed) Step 2: Practice – Interactive Problem Drill Step 3: Recap – Super Review Cheat Sheet 69/67 Go for it! http://www.RapidLearningCenter.com
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