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A scientifically untrained but curious friend asks, "When I walk into a room. is there a chance that all the air will be on the other side?" How do you answer this question?

Short Answer

Expert verified
Theoretically, it's possible for all air in a room to end up on one side purely by chance, but the probability of this occurring is so small due to the sheer number and random motion of the gas molecules. Hence, for all practical purposes, it is considered impossible.

Step by step solution

01

STEP 1: Understand Gas Behavior

First, introduce the concept that gases fill the available space evenly due to the continue motion of their molecules. The molecules of air are in constant, random motion and are likely to be spread out evenly in a room. This is a fundamental principle of gas behavior that can be deduced from the Kinetic Gas Theory.
02

STEP 2: Explain Unlikely Scenarios

Although it's theoretically possible for all the gas molecules to end up on one side of the room purely by chance (since their motion is random), the probability of this happening is infinitesimally small due to the vast number of molecules involved. This aligns with the principle of statistical mechanics that systems tend to evolve towards the most probable arrangements.
03

STEP 3: Quantify The Low Probability

Although it's difficult without concrete numbers, help them appreciate just how unlikely this scenario is. Compare it with other highly unlikely events like winning the lottery, but stress that it is still a much smaller likelihood than that.

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Key Concepts

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

Understanding Gas Behavior
When considering how gases like the air around us behave, there's a fascinating principle at play. Air consists of a myriad of tiny particles called molecules, which are perpetually on the move. This constant movement is not random chaos; rather, it stems from the inherent energy of the particles, what scientists refer to as kinetic energy. The Kinetic Gas Theory illustrates that these energetic particles collide with each other and the walls of their container—in this case, the room—and as a result, spread out to fill the entire available space.

Imagine a crowd exiting a concert hall; naturally, people disperse out of the exits and eventually spread across the wider outside area. Similarly, gas molecules disperse throughout an entire room. This behavior is predictable and underpins why we can confidently enter a room knowing that the air won't be lumped awkwardly in one corner. It also gives us a base to understand more intricate gas properties, such as pressure and temperature, which are directly tied to molecular motion and collisions.
Statistical Mechanics: Navigating the Sea of Possibilities
In the realm of tiny particles, statistical mechanics takes the stage by utilizing the power of mathematics and probability to predict the behavior of particle systems. It acknowledges that while individual particles follow the laws of physics, their collective behavior can be better understood statistically. This branch of physics considers all possible arrangements of a system's particles and determines which configurations are the most probable.

Our scenario of a room filled with air is a practical application of statistical mechanics. Among the astronomical number of potential arrangements of air molecules, the overwhelming majority have those molecules dispersed uniformly. It's statistically inevitable that this is how we find the air in any room we walk into. Granted, a minuscule chance exists where all molecules could decide to 'hang out' on one side, but statistical mechanics assures us that such an event is so unlikely it verges on the impossible.
Probability in Physics: Why Winning Isn't Everything
Physics often involves predicting the likelihood of different events, and probability is the mathematical tool that makes this possible. By calculating the odds of various outcomes—like a coin landing heads or tails—we can form expectations around what should happen in a given scenario. Our question about all the air being on one side of the room is a classic probability problem.

Let's put this into perspective: The probability of such an event is extraordinarily low, far less than your chance of winning the lottery or being struck by lightning. In the realm of physics, particularly when dealing with vast numbers of particles, there are degrees of unlikely. Some events, while theoretically possible, are so improbable that for all practical considerations, they can be deemed impossible. The exceedingly low probability of all air molecules being on one side of a room is an example of just such an event, serving as a perfect illustration of probability at work in physics.

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Most popular questions from this chapter

This problem investigates what fraction of the available chayge must he tranferred from one conductor to another to produre a typical contact potential. (a) As a rough appnximation, treat the conductors as \(10 \mathrm{~cm} \times\) \(10 \mathrm{c} \mathrm{m}\) square plates \(2 \mathrm{~cm}\) apart - a parallel-plate capactor \(-\) so that \(q=C V\), where \(C=\varepsilon_{\mathrm{p}}\left(0.01 \mathrm{~m}^{2} / 0.02 \mathrm{~m}\right)\). How much charge must be iransferred from one plate to the other to produce a potential difference of \(2 \mathrm{~V}\) ? (b) Approximately what fruction would this be of the total number of conduction electrons in a \(100 \mathrm{~g}\) piece of copper, which has one conduction electron per atem?

Determine the relative probability of a gas molecule being within a small range of speeds around \(2 {\text {rms }}\) to being in the same range of speeds around \(v {_\text {rms }}\).

Figure 9.8 cannot do justice to values at the very high. speed end of the plot. This exercise investigates how small it really gets. However, although integrating the Maxwell speed distribution over the full range of speeds from 0 to infinity can be carried out (the so-called Gaussian integrals of Appendix \(K\) ). over any restricted range, it is one of those integrals that. unfortunately. cannot be done in closed form. Using a computational aid of your choice, show that the fraction of molecules moving faster than \(2 v_{\text {ms }}\) is \(\sim 10^{-2}\); faster than \(6 v_{\text {ms }}\) is \(-10^{-23} ;\) and faster than \(10 v_{\mathrm{ms}}\) is \(\sim 10^{-64}\), where \(v_{\mathrm{m} 2}\) from Exercise \(41 .\) is \(\sqrt{3 k_{B} T / m}\). (Exercise 48 uses these values in an interesting application.)

Consider the two-sided room, (a) Which is more likely to have an imbalance of five particles (ie., \(N_{\mathrm{k}}=\frac{1}{2} N+5\) ): a room with \(N=20\) or a room with \(N=60\) ? (Note: The total number of ways of distributing particles, the sum of \(W_{N_{k}}^{N}\) from \(O\) to \(N,\) is \(2^{N}\).) (b) Which is more likely to have an imbalance of \(5 \%\) (i.e., \(\left.N_{R}=\frac{1}{2} N+0.05 N\right) ?\) (c) An average-size room is quite likely to have a trillion more air molecules on one side than on the other. Why may we say that precisely half will be on each side?

A block has a cavity inside, occupied by a photon gas. Briefly explain what the characteristics of this gas should have to do with the temperature of the block.

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