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Thermodynamics Honors Physics.

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Presentation on theme: "Thermodynamics Honors Physics."— Presentation transcript:

1 Thermodynamics Honors Physics

2 Biblical Reference Job 41:31
It makes the depths churn like a boiling caldron and stirs up the sea like a pot of ointment. Job 41:31

3 Work done by a gas If a piston is filled with a specific amount of gas, as you add heat, the temperature rises and the volume of the gas expands. The gas applies a force on the piston wall pushing it a specific displacement. Thus, a gas can do work (Force x Distance).

4 Work is the AREA of a P vs. V graph

5 The Sign in the Work Equation
Since work done by a gas has a positive volume change, the gas is using up energy (or losing energy) thus the negative sign. When work is done on a gas the change in volume is negative. This cancels out the negative sign in the equation, because some external agent is adding energy to the gas.

6 Zeroth Law of Thermodynamics
If Objects A and B are independently in thermal equilibrium with Object C, then Objects A and B are in thermal equilibrium with each other. Why “Zeroth”? It was formed after 1st, 2nd, and 3rd, but was more fundamental.

7 First Law of Thermodynamics
“The internal energy of a system tends to increase when HEAT is added and work is done ON the system.” If you ADD heat then transfer work TO the gas, the internal energy must go up, because you have MORE than what you started with.

8 Example Sketch a PV diagram and find the work done by the gas during the following stages. A gas is expanded from a volume of 1.0 L to 3.0 L at a constant pressure of 3.0 atm. The gas is then cooled at a constant volume until the pressure falls to 2.0 atm 600 J

9 Example continued The gas is then compressed at a constant pressure of 2.0 atm from a volume of 3.0 L to 1.0 L. The gas is then heated until its pressure increases from 2.0 atm to 3.0 atm at a constant volume. -400 J

10 Example continued What is the NET WORK?
600 J J = 200 J NET work is the area inside the shape. Rule of thumb: If the system rotates CW, the net work is positive. If the system rotates CCW, the net work is negative.

11 Thermodynamic Processes - Isothermal
To keep the temperature constant both the pressure and volume change to compensate. Volume goes up, pressure goes down “BOYLES’ LAW”

12 Boyle’s Law Boyle’s law states that when temperature is constant:
Pressure of a gas increases if the volume decreases. Pressure of a gas decreases if the volume increases.

13 Pressure & Volume Pressure and Volume are inversely proportional.

14 Boyle’s Law – Solve for V2
If you add 15 L of air to a balloon at sea level (101 kPa) and then take the balloon to Denver, where the air pressure is 86 kPa, what will be the new volume of the balloon? P2 P2

15 Boyle’s Law – Solve for P2
If you have 5.6 liters of gas in a piston at a pressure of 152 kPa and compress the gas until its volume is 4.8 L, what will be the new pressure inside the piston? V2 V2

16 Boyle’s Law – P1V1 = P2V2 Calculate the pressure in atmospheres in a motorcycle engine at the end of the compression stroke. Assume that at the start of the stroke, the pressure of the mixture of gasoline and air in the cylinder is mm Hg and the volume of each cylinder is mL. Assume that the volume of the cylinder is mL at the end of the compression stroke.

17 Thermodynamic Processes - Isovolumetric
Gas undergoes a temperature change but no change in volume. No work is done on or by the system. Gay-Lussac’s Law

18 Gay-Lussac’s Law - A container is designed to hold a pressure of 2.5 atm. It is filled with air at room temperature (20°C – 293 K) and normal atmospheric pressure. Would it be safe to throw the container into a fire where temperatures of 600°C (873 K) would be reached?

19 Thermodynamic Processes - Isobaric
Heat is added to the gas which increases the Internal Energy (U). Work is done by the gas as it changes in volume. The path of an isobaric process is a horizontal line called an isobar. ∆U = Q - W can be used since the work is positive. Charles’ Law

20 Charles’ Law Charles’s law states that when the pressure is constant:
The volume of a gas increases if the temperature increases. The volume of a gas decreases if the temperature decreases.

21 Temperature and Volume
Volume and Temperature are directly proportional.

22 Charles’ Law – Solve for V2
If you have 45 L of helium in a balloon at 25 C (298 K) and increase the temperature of the balloon to 55 C (328 K), what will be the new volume of the balloon?

23 Charles’ Law – Solve for T2
If you have 130 L of gas in a piston at 250 C (523 K), and cool the gas until the volume decreases to 85 L, what will be the temperature of the gas?

24 Charles’ Law - Assume that the volume of a balloon filled with H2 is L at 25°C. Calculate the volume of the balloon when it is cooled to -78°C in a low-temperature bath made by adding dry ice to acetone.

25 Thermodynamic Processes - Adiabatic
Greek - adiabatos- "impassable" No heat can leave or enter the system. Work is done and internal energy changes but heat does not change.

26 Combined Gas Law - A sample of gas has a volume of 283 mL at 25C (298 K) and atm. What is the volume at 100C (373 K) and 1.00 atm?

27 In Summary Gay-Lussac’s Law Charles’s Law

28 Example A gas is enclosed in a container fitted with a piston of cross sectional area .10 m2. The pressure of the gas is maintained at 8000 Pa while the heat is slowly added, pushing the piston up a distance of .04 m. If 42 J of heat is added to the system during the expansion, what is the change in internal energy?

29 Second Law of Thermodynamics
“Heat will not flow spontaneously from a colder body to a warmer body AND heat energy cannot be transformed completely into mechanical work.” The bottom line: Heat always flows from a hot body to a cold body Nothing is 100% efficient

30 Heat Engines QH = remove from, absorbs = hot
Convert thermal energy into mechanical energy. QH = remove from, absorbs = hot QC= exhausts to, expels = cold Heat flows from a Hot reservoir to a Cold reservoir

31 Engine Efficiency In order to determine the thermal efficiency of an engine you have to look at how much energy you get out based on how much energy you take in.

32 Example – Engine Efficiency
An automobile engine has an efficiency of 22.0% and produces 2510 J of work. How much heat is rejected by the engine?

33 Rates of Energy Usage Sometimes it is useful to express the energy usage of an engine as a RATE. For example: The RATE at which heat is absorbed. The RATE at which heat is expelled. The RATE at which WORK is DONE.

34 Is there an IDEAL engine model?
How efficient can an Engine be? What’s the most work we can possibly get for a given amount of fuel? The efficiency question was first posed - and solved - by Sadi Carnot in 1820, not long after steam engines had become efficient enough to begin replacing water wheels, the main power sources for industry.  Carnot visualized the heat engine as a kind of water wheel in which heat (the “fluid”) dropped from a high temperature to a low temperature, losing “potential energy” which the engine turned into work done, just like a water wheel. 

35 Entropy – the Measure of Disorder
Greater disorder means there is less energy to do work.

36 Example – Tropical Ocean as a Heat Engine
Water near the surface of a tropical ocean has a temperature of K (25.0 ºC), whereas water 700 m beneath the surface has a temperature of K (7.0 ºC). It has been proposed that the warm water may be used as the hot reservoir and the cool water as the cold reservoir of a heat engine. What would be the efficiency for such an engine. TH = K and TC = K

37 Cooling and Heating Systems

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