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Chapter 5 Textbook Readings and Problems
For all editions read the sections labeled: Gas Stoichiometry Dalton's Laws of Partial Pressures The Kinetic Molecular Theory of Gases Real Gases |
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I didn't really care for the problems at the end of the chapter. They seemed rather plain (boring). So I created my own that cover many of the same type of problems but with more interesting subject matter. This chapter is all about gases and there's a lot of interesting things that can be done with gases. For one, compressed air can be a source of energy for transportation.. The first few problems relate to this new development. | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
There are a few cars in production that run from air. This is the Airpod car. It's powered by compressed air. So there's no pollution. I think these cars are good for us in Arizona because as the compressed air becomes uncompressed as it goes through the engine and out the "exhaust" pipe, the air gets cold. This will give us free air conditioning. The compressed air is stored in high-strength and low weight carbon-fiber tanks. | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
This guy took that idea and made an air powered bicycle from two 16.0-liter carbon-fiber tanks. They can easily hold 3,000 psi (3.00x103psi) of pressure. Problem 1: What is the weight in grams (cell V2) of each tank if the air is 3,000 psi with a temperature of 77.0°F and the empty weight of tank is 10.0 lbs? Air is a mixture of 20% oxygen and 80% nitrogen, with molar masses of 32 g/mole O2 and 28g/mole N2. If we take 80% of 28g/mole and add 20% of 32g/mole, we get 28.8g/mole. So together they act like a gas that is 28.8 g/mole. So if we find the number of moles in a 16 liter tank, we can turn that into grams. We begin with PV=nRT, and we solve for moles(n). Divide both sides by RT and we get: PV/RT=n. That can also be written as PV/R/T=n |
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Remember because our constant (R) has units of atm·Liter/mole·K, we need the psi converted to atm and the 77°F turned into Kelvin.
Problem 2: What is the number that goes into C3? |
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This is another car that is powered by air. Its carbon-fiber cylinders have a volume of 800 liters and weigh 75 lbs when empty. The temperature is 65°F and the pressure in the tanks is 3650 psi. We can use the spreadsheet above to calculate the weight of the tanks. Problem 7: What cells need to be updated to do that? |
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The fire piston was invented by people in the southeast asia and Indonesia over a thousand years ago. The principle is that compression of gas will cause the gas to heat up. The same principle is used in diesel engines to ignite the fuel. If done quickly, the heat doesn't have time to be lost and is retained in the cylinder. My colleagues and I debated about how this compression actually makes the air hotter. I used a spreadsheet to calculate the speed one molecule would speed up if bouncing back and forth from the top to bottom of the cylinder as a piston came down. Each time the molecule hit the moving piston it bounced back a little faster. By the time the piston moved to about 1 cm from the bottom, that molecule had bounced off the moving piston many times making the molecule move at speeds equivalent to temperatures over a 1000°F. |
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The volume of the air in the fire piston cylinder starts at 10.0 mL and then is squeezed to 1.0 mL. The temperature started as 25°C (room temp) and ended up at 600.°C. The pressure before being squeezed was 740mm of mercury (Note 760mm Hg is 1 atmosphere). We want the final pressure. If temperature had remained the same, this would be easy. The volume went down to 1/10 its original size, which would make the pressure be 10 times larger (740mm x 10=7,400mm mercury). However, the temperature changed, so it's more complicated. We can start with PV=nRT; however, there are two conditions. One at the beginning and one at the end. So we need two PV=nRT formulas. Let P1V1=n1RT1 be the values before it was compressed. Then P2V2=n2RT2 would be the values after compression and becoming hot. Since R is constant, it is the same in both equations. We can exploit that fact. Let's solve both equations for R. In the first R=P1V1/n1T1, and the second is R=P2V2/n2T2. Since both are equal to R, they are equal to each other. So, P1V1/n1T1=P2V2/n2T2. Since the moles of the gas didn't change, n1=n2, we can multiply both sides by n1, which would cancel out both n1 and n2. Our equation now reads: P1V1/T1=P2V2/T2 We know all of these values except for P2 (final pressure). So lets solve for P2 by dividing both sides by V2 and multiplying both sides by T2. We now get P1V1T2/(T1V2)=P2, which can also be written as P1x V1x T2 /T1 /V2=P2. This looks like a good job for a spreadsheet. Since there's no R in the formula, we don't need pressure measured in atmospheres or volume in liters, but we do have to use Kelvin. So 273 gets added to the Celsius degrees. The units in red cancel out. |
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Problem 8: What is the final pressure in mm of mercury (mm of Hg)? Problem 9: What is the formula that goes in L2? Problem 10: What would be the final pressure if the end volume was 0.7mL? |
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The pressure in the fire piston will go up at the point the tender attached to the bottom of the pistion catches fire. (I used a piece from a cotton ball in my fire piston). When the cotton burns, it will consume the oxygen but will produce carbon dioxide and water vapor and higher temperatures. So the pressure should go up due to more gases and higher temperature. 2C6H12O5+13O2 --> 12CO2 + 12H2O We can't ignore the nitrogen gas, which is 5 times the number of oxygen molecules (5 x 13=65). So we can add that to the reaction. Looking at this we see that we start with 78 moles (12+65) of gases and end with 84 moles (12+12+65) of gases. Also, the burning will increase the temperature. The yellow flame indicates a temperature around 3,000 Kelvin. |
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This problem is similar to the last one but the intitial conditions are the final conditions in the above problem. After the flame heats up the air and creates the extra gases, the condition is different. Let's use P3V3=n3RT3 for the new final condition. Like before we can solve for R on both and set them equal to each other. This looks like the last time we did it: This time the moles are changing, but the volume is the same. So we need to keep the moles (n2 and n3) but we can drop the volumes. That simplifies it to: Solving for the final pressure (P3) by multiplying both sides by n3 and T3 gives us: Even though we don't know the exact number of moles, we do know the ratio of moles, which works fine when you have one divided by the other. So the 78 moles for n2 and the 85 moles for n3 that we got from the balanced equation works fine.
We can check the units to see if they cancel and we can check the logic. In the above spreadsheet we see that we have 85 moles over 78 moles. So that's 85/78, which will make the pressure larger as expected. We see the temperature ratio of 3000 over 873 or 3000/873, which will also make the pressure larger. So these fractions are doing what we expect should happen to the pressure which is to become larger when there's more moles and higher temperatures. |
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When I heard about the runaway balloon that might be carrying a 50 lb boy, I wondered if the balloon was big enough to lift him. I started doing some calculations. You need to know the weight of the helium that fills the balloon and the weight of air of that same volume. The difference will be the lift. I knew the volume of a sphere has the formula of 4/3pi x r3. This one is flattened. So you use the radius going front to back, side to side and top to bottom. In the news they said it had a 20 foot diameter and was 5 feet tall. That means the radius side to side was 10 ft and front to back was also 10 ft. The top to bottom radius was 2.5 ft. Once you get volume you need to know the mass of that volume in helium and in air. We can look it up or use the 22.4 liters=1 mole of a gas at STP (standard temperature and pressure of 0°C and 1 atmosphere). | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
Since the volume formula usng feet will create cubic feet, we need to lookup on the Internet the conversion of cubic ft to liters. Air is nitrogen and oxygen, but weighs 28.8 grams per mole of those molecules (we did it earlier). So we can use that to change moles to grams.
At this point you will have the pounds of lift that the balloon is capable of; however, you would have to estimated the weight of the balloon fabric and the bottom instrument box in order to know what the actual lifting capability of the balloon. Problem 13: Was this balloon capable of carrying that 50lb boy? |
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Send answers to Ken Costello at chm151@chemistryland.com. Use a subject line of Chapter 5. |
Update 4/22/10