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Ideal gas particles are assumed to be volume less and to neither attract nor repel each other. Why are these assumptions crucial to the validity of Dalton’s law of partial pressures?

Short Answer

Expert verified
The assumptions of ideal gas particles being volumeless and having no interactions are crucial to the validity of Dalton's Law of Partial Pressures because they simplify the behavior of gas particles, allowing scientists to predict and calculate gas properties. By assuming gas particles have no volume and interactions, we can treat each particle independently and simply add their partial pressures together, without any complications due to their size or interaction, to get the total pressure as described by Dalton's Law: \(P_{total} = P_1 + P_2 + \cdots + P_n\). Without these assumptions, accurately predicting the total pressures of mixed gases using Dalton's Law would be much more difficult.

Step by step solution

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1. Understanding Ideal Gas Assumptions

The Ideal Gas Law (PV = nRT) is based on two key assumptions: (a) gas particles have no volume compared to the space between them, and (b) gas particles have no interactions with each other (neither attractive nor repulsive forces). These assumptions simplify the behavior of gas particles, allowing scientists to predict and calculate gas properties.
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2. Dalton's Law of Partial Pressures

Dalton's Law states that in a mixture of ideal gases, the total pressure is equal to the sum of the partial pressures of the individual gas components. Mathematically, we can write it as: \(P_{total} = P_1 + P_2 + \cdots + P_n\) Where \(P_{total}\) is the total pressure, and \(P_1, P_2, \cdots, P_n\) are the partial pressures of the individual gas components.
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3. Volumeless Gas Particles

The assumption of volumeless gas particles is important for the validity of Dalton's Law because it allows gas particles to be considered independently without worrying about their size. As the particles are assumed to be volumeless, their contribution to the total pressure is dependent only on the forces they exert on the container walls and not on the sizes of particles. This means each particle can be treated independently, and their partial pressures can be added up to get the total pressure.
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4. No Interactions Between Gas Particles

The assumption of no interaction between gas particles is also crucial to the validity of Dalton's Law because it prevents any interference between the particles that could affect their contribution to the total pressure. If gas particles attracted or repelled each other, their pressures wouldn't be independent, and they couldn't be added together as simply as in Dalton's Law.
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5. Conclusion

The assumptions of ideal gas particles being volumeless and having no interactions are crucial to the validity of Dalton's Law of Partial Pressures because they allow the pressure of individual gas particles to be added together without any complication due to their size or interaction. If the assumptions didn't hold, it would be much more difficult to accurately predict the total pressures of mixed gases using Dalton's Law.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Ideal Gas Law Assumptions
The Ideal Gas Law is based on certain assumptions that simplify the study and understanding of gases. These assumptions include:
  • Gas particles are assumed to have no volume. This means their size is negligible compared to the space they occupy.
  • Gas particles are assumed to exert no forces on each other, meaning there are no attractions or repulsions between them.
These assumptions are necessary for the law to function predictably. They allow scientists to create models that successfully predict how gases behave under different conditions. In real-world applications, these assumptions help in simplifying calculations and understanding gas mixtures, like those found in air.
Ideal Gases
Ideal gases are hypothetical gases that perfectly adhere to the gas laws, including the Ideal Gas Law (PV = nRT). Their behavior is predictable because they follow specific assumptions:
  • They move with constant velocity.
  • They don’t interact with each other.
  • Their collisions are perfectly elastic, meaning no energy is lost.
In reality, no gas is truly ideal. However, most gases behave as ideal gases under many conditions, such as at high temperatures and low pressures. This ideal behavior allows scientists and chemists to use simple calculations to predict and understand various gas-related phenomena.
Partial Pressures
Partial pressures refer to the pressure exerted by an individual gas within a mixture of gases. According to Dalton's Law of Partial Pressures, the total pressure of a gas mixture is the sum of the partial pressures of all the individual gases in the mixture.
This can be mathematically expressed as:
\[ P_{total} = P_1 + P_2 + ext{...} + P_n \]
Each gas in a mixture acts independently when applying Dalton’s Law, assuming ideal gas behavior. The pressure each gas contributes is directly related to its proportion in the mixture. Without considering interactions or volume, the task of calculating total pressure becomes straightforward by adding up each partial pressure.
Gas Particle Interactions
When considering gas particle interactions, it's important to know that ideal gases assume no interactions between particles. This means:
  • No attractive forces: Particles do not pull towards each other.
  • No repulsive forces: Particles do not push away from each other.
These assumptions ensure that each gas in a mixture contributes independently to the total pressure. If gas particles interacted, either by attraction or repulsion, their behavior and, subsequently, the pressure they exert would change. This would violate Dalton’s Law, as the partial pressures would not be truly additive. Understanding that no interactions occur simplifies the estimation of pressures in complex gas mixtures.

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Most popular questions from this chapter

In 1897 the Swedish explorer Andreé tried to reach the North Pole in a balloon. The balloon was filled with hydrogen gas. The hydrogen gas was prepared from iron splints and diluted sulfuric acid. The reaction is $$\mathrm{Fe}(s)+\mathrm{H}_{2} \mathrm{SO}_{4}(a q) \longrightarrow \mathrm{FeSO}_{4}(a q)+\mathrm{H}_{2}(g)$$ The volume of the balloon was 4800 \(\mathrm{m}^{3}\) and the loss of hydrogen gas during filling was estimated at \(20 . \%\) . What mass of iron splints and 98\(\%\) (by mass) \(\mathrm{H}_{2} \mathrm{SO}_{4}\) were needed to ensure the complete filling of the balloon? Assume a temperature of \(0^{\circ} \mathrm{C},\) a pressure of 1.0 atm during filling, and 100\(\%\) yield.

Hydrogen azide, \(\mathrm{HN}_{3},\) decomposes on heating by the following unbalanced equation: $$\mathrm{HN}_{3}(g) \longrightarrow \mathrm{N}_{2}(g)+\mathrm{H}_{2}(g)$$ If 3.0 atm of pure \(\mathrm{HN}_{3}(g)\) is decomposed initially, what is the final total pressure in the reaction container? What are the partial pressures of nitrogen and hydrogen gas? Assume the volume and temperature of the reaction container are constant.

A compound containing only \(\mathrm{C}, \mathrm{H},\) and \(\mathrm{N}\) yields the following data: i. Complete combustion of 35.0 \(\mathrm{mg}\) of the compound produced 33.5 \(\mathrm{mg}\) of \(\mathrm{CO}_{2}\) and 41.1 \(\mathrm{mg}\) of \(\mathrm{H}_{2} \mathrm{O} .\) ii. A 65.2 -mg sample of the compound was analyzed for nitrogen by the Dumas method (see Exercise \(137 ),\) giving 35.6 \(\mathrm{mL}\) of dry \(\mathrm{N}_{2}\) at \(740 .\) torr and \(25^{\circ} \mathrm{C}\) . iii. The effusion rate of the compound as a gas was measured and found to be \(24.6 \mathrm{mL} / \mathrm{min}\). The effusion rate of argon gas, under identical conditions, is \(24.6 \mathrm{mL} / \mathrm{min}\). What is the molecular formula of the compound?

The average lung capacity of a human is 6.0 L. How many moles of air are in your lungs when you are in the following situations? a. At sea level \((T=298 \mathrm{K}, P=1.00 \mathrm{atm})\) b. \(10 . \mathrm{m}\) below water \((T=298 \mathrm{K}, P=1.97 \mathrm{atm})\) c. At the top of Mount Everest \((T=200 . \mathrm{K}, P=0.296 \mathrm{atm})\)

An ideal gas is contained in a cylinder with a volume of \(5.0 \times\) \(10^{2} \mathrm{mL}\) at a temperature of \(30 .^{\circ} \mathrm{C}\) and a pressure of 710 . torr. The gas is then compressed to a volume of 25 \(\mathrm{mL}\) , and the temperature is raised to \(820 .^{\circ} \mathrm{C}\) . What is the new pressure of the gas?

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