Combined Gas Law and Demonstrations
Aluminum Can Crush Demonstration
- Initial state: Plain aluminum can with a small amount of water at the bottom.
- Heating: The can is heated until the water boils.
- Observation: Adding heat increases the kinetic energy of the water molecules, raising the temperature.
- Rapid Cooling: The heated can is flipped into an ice bath, causing a sudden temperature change.
- Result: The can is crushed rapidly due to the change in pressure.
Analysis of the Can Crush
- Initial Conditions:
- Air pressure (atmospheric pressure) is present.
- Water is in the liquid phase at room temperature.
- Heating Phase:
- The can is open, allowing air (and thus air pressure) to move in and out.
- Applying heat causes the water to boil, releasing water vapor (gas molecules) into the can and escaping as steam.
- Sealing and Cooling:
- Flipping the can into the ice bath seals the container, preventing steam from escaping.
- The environment rapidly changes from hot to cold.
- Water molecules rapidly lose kinetic energy.
- Pressure Change:
- The rapid cooling causes a pressure drop inside the can.
- Initially, atmospheric pressure is balanced by the pressure inside the can (due to the escaping gas particles).
- After sealing and cooling, the internal pressure decreases.
- External Pressure:
- Atmospheric pressure remains constant on the outside of the can.
- Volume Reduction:
- The external atmospheric pressure exceeds the internal pressure.
- This pressure difference causes the can to be crushed, reducing its volume.
- It's not that water is sucked in but rather external pressure forces the can to collapse.
- Relationship: The demonstration illustrates the inverse relationship between pressure and volume.
Combined Gas Law
- The combined gas law integrates all individual gas laws into a single equation.
- Equation: n<em>1T</em>1P<em>1V</em>1=n<em>2T</em>2P<em>2V</em>2
- Variables:
- P = Pressure
- V = Volume
- n = number of moles
- T = Temperature
- Individual Gas Laws:
- Boyle's Law: P<em>1V</em>1=P<em>2V</em>2 (at constant n and T)
- Charles's Law: T</em>1V<em>1=T</em>2V<em>2 (at constant n and P)
- Gay-Lussac's Law: T</em>1P<em>1=T</em>2P<em>2 (at constant n and V)
- Avogadro's Law: n</em>1V<em>1=n</em>2V<em>2 (at constant T and P)
- Usage: By canceling out constant variables, the combined gas law can be simplified to solve various gas problems.
Example Problem 1
- Problem: 3.00 L of a gas is collected at 35°C and 765 mmHg. What is the volume at STP?
- Givens:
- V1 = 3.00 L
- T1 = 35°C = 308 K (35 + 273)
- P1 = 765 mmHg
- STP (Standard Temperature and Pressure):
- T2 = 0°C = 273 K
- P2 = 1 atm = 760 mmHg
- Unknown: V_2
- Since the amount of gas is not changing, n can be removed from the combined gas law.
- Simplified Equation: \frac{P1V1}{T1} = \frac{P2V2}{T2}
- Plug in the values: \frac{(765)(3.00)}{308} = \frac{(760)V_2}{273}
- Cross multiply and solve for V_2
- (765 \times 3 \times 273) = 626535
- (308 \times 760) = 234080 V_2
- V_2 = \frac{626535}{234080} = 2.68 L
Example Problem 2
- Problem: A flexible container contains 0.76 moles of helium at 31°C and 16.5 L. If 0.22 moles of helium is released, what is the new volume at the same temperature and pressure?
- Givens:
- n_1 = 0.76 moles
- T_1 = 31°C = 304 K
- V_1 = 16.5 L
- n_2 = 0.76 - 0.22 = 0.54 moles (amount left after release)
- TandP are constant.
- Unknown: V_2
- Simplified Equation (since TandPareconstant):\frac{V1}{n1} = \frac{V2}{n2}
- Plug in the values: \frac{16.5}{0.76} = \frac{V_2}{0.54}
- Cross multiply and solve for V_2
- 16.5 \times 0.54 = 8.91
- 0.76 \times V_2
- V_2 = \frac{8.91}{0.76} = 11.7 L \approx 12 L
- Result: V_2 \approx 12$$ liters (rounded to two significant figures)