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Thermodynamics

Thermodynamics. Energy from chemical bonds is converted to kinetic energy and heat (body and friction from tires). ENERGY. Heat. 1 st law of thermodynamics. Energy may be converted to different forms, but it is neither created nor destroyed during transformations.

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Thermodynamics

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  1. Thermodynamics

  2. Energy from chemical bonds is converted to kinetic energy and heat (body and friction from tires) ENERGY Heat 1st law of thermodynamics Energy may be converted to different forms, but it is neither created nor destroyed during transformations Amount of energy before and after transformation is the same, only the form of the energy has changed

  3. 1st Law (Contd.) Example: Can make wood hotter by applying fire or hitting Another way to state the 1st law is mathematically. DE = Q + W This equation says that the only way to change the energy of a system is to add heat to it (Q) or to do work on it (W)

  4. Heat While used a lot in our vocabulary, this term is very misunderstood Heat - the ENERGY transferred between objects of different temperature Heat is NOT temperature. An object CANNOT contain heat; objects contain thermal energy. Heat is a very important type of energy transfer

  5. Heat Versus Temperature Temperature - the property that two objects have in common when NO heat is transferred between them Temperature is a relative property. We define it in relationship to other things T1 > T2 T1 = T2

  6. Heat Flow Heat can flow via one of three methods • Conduction - energy transfer by next-nearest molecule interaction • Convection - energy transfer by mixing; can be naturalor forced (fan, stirring, etc.) • Radiation - energy transfer by electromagnetic radiation

  7. Conduction Energy transfer by nearest molecules running into each other Rate of heat transfer depends on • Temperature difference DT = TH - TC • Thickness of material L • Thermal conductivity of material k • Surface area A Q k DT A = t L

  8. Conduction More familiar Q DT A = t R If intervening material is made up of more than one substance, add R-values Rtotal = R1 + R2 + R3 + …. Problem: How is the rate of heat transfer affected by adding anR-value 8 insulation to an 8’x20’ wall that has an R-value of 12when the temperature difference is 20 oF?

  9. Convection Heat transfer via mixing; requires some type of fluid (gas, liquid) Things can naturally convect, especially when density changesand more buoyant materials will rise Forced convection requires energy input

  10. Radiation Every object in the universe emitselectromagnetic radiation because it has a temperature above absolute zero. Type of radiation depends upon the value of the temperature .003 m K Wein’s Law => lmax = T Problem: At what wavelength do you emit most of your radiation?

  11. Stefan-Boltzmann Law The rate of heat emission due to radiation depends on size and temperature. Q/t = e s A T4 where e is the emissivity of the object Remember, the object will be absorbing radiation while it isemitting. Therefore, the total heat transfer is Q/t = e s A (Tobject4 - Tsurroundings4)

  12. Heat Transfer Devices Heat Pump Heat Engine Outputs useful energy W by extracting it from heat passing from hot to cold Example: Car engine Transfers heat from cold to hot using external energy W Example: Refrigerator In both devices, QH = QC + W

  13. ANSWER: Although energy isn’t destroyed, in every energy transfer, some of it will change to a non-usable form 2nd law of thermodynamics If energy is never created or destroyed, why can’t we keep reusing the same energy source forever? This is a consequence of the 2nd law of thermodynamics “In a closed system, the total entropy either increases or stays the same”

  14. Waste Heat ENERGY Second law of thermodynamics When a chemical bond is broken, you get some high quality ENERGY capable of doing work, and some low quality “wasted” energy No energy was lost or created in the transfer, but the usability of the energy declined in the transformation. This low quality energy cannot be effectively harnessed to do any more work, so you cannot use one energy source forever

  15. Second law of thermodynamics Example: powering your car Breaking chemical bonds in gas during combustion yields high quality energy which produces kinetic energy to move car Also produces waste energy as heat with little ability to do work

  16. Combustion of gasoline Piston movement Axle turns Wheels turn Energy in gasoline E E E E E E E E Friction with axle Friction of tires with road Heat loss during combustion Friction with pistons Usable E Amount of high quality energy declines with each step (width of orange arrows) No energy is lost, it simply is converted to low-quality heat that cannot be used for further work

  17. Efficiency A measure of how well energy is converted useful energy out Efficiency = total energy input Examples Internal combustion engine car is about 10% efficient Electric car is about 20% efficient Incandescent light bulb is about 1% efficient

  18. Efficiency Example 30,000 J = .375 = 37.5 % Efficiency = 80,000 J = 10,000 J A power plant consumes 80,000 Joules of coal energy to produce 30,000 Joules of electricity. What is the efficiency?

  19. Heat Engine Efficiency Energy input = QH Usable energy output = W W Efficiency = QH Since QH = QC + W => W = QH - QC QC Efficiency = 1 - QH Problem: A car takes in 20,000 J of gasoline and outputs 19,000 J of heat. What is the efficiency of the car?

  20. Heat Pump COP For heat pumps, it is not proper to discussefficiency since there is no “usable energyouput”. Instead, define “coefficient of performance” to discuss how much energyit moves per energy paid for. QH COPheater = W QC COPa.c. = W Note: COPheater is always greater than 1. Why?

  21. Maximum Efficiency TC Maximum efficiency = 1 - TH Unfortunately, the 2nd law of thermodynamics limits the maximum efficiency that a device can have. No device will ever be 100% efficient. For a heat engine, the limit is given by where TC is the temperature of the cold reservoir and TH is the temperature of the hot reservoir in the Kelvin temperature scale

  22. Maximum Efficiency Example 278 K = 1 - .95 = .05 Maximum efficiency = 1 - 293 K An inventor proposes a heat engine that will produce electricity by extracting heat from ocean surface water at 20oC (293 K) and dumping the waste heat to the deep ocean at 5oC (278 K). What is the maximum efficiency? At most, this device will be 5% efficient. In reality, it will probably only be about half of this, or 2-3% efficient.

  23. 1st LAW: Energy is neither created nor destroyed, only transformed 2nd LAW: Energy is transformed from high quality to low quality RESULT: Low quality heat cannot do substantial work, requiring a new source of high quality energy Recapping

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