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Pressures, law of partial

Many gas samples, including our atmosphere, are mixtures that consist of different kinds of gases. The total number of moles in a mixture of gases is [Pg.420]

Unless otheiwise noted, all content on this page is Cengage Learning. [Pg.420]

Now fifJiT/V is the partial pressure that the % moles of gas A alone would exert in [Pg.421]

The total pressure exerted by a mixmre of ideal gases is the sum of the partial pressures [Pg.421]

Dalton s Law is useful in describing real gaseous mixtures at moderate pressures because it allows us to relate total measured pressures to the composition of mixtures. [Pg.421]

Another concept you have to understand is mole fraction. The mole fraction of a gas is the fraction or ratio of moles of that particular gas against the total number of moles of gases present in the mixture. Mole fraction is defined as follows  [Pg.84]

A 1 liter flask contains 0.4 mol of helium and 1.2 moles of hydrogen gas. Find the mole fractions and partial pressures of both gases, if the total pressure of the mixture is 790 mmHg. [Pg.84]

The total number ofmolesof ses present in the container is 0.4+ 1.2= 1.6 moles [Pg.84]

Notice that die sum of the mole fractions is always one. If it is not, you probably made an error somewhere in your calculation. Here, [Pg.84]

we have to find the partial pressures of the gases. We know that the partial pressures of the gases should add up to get the total pressure of the gases. Now that we know the total pressure and the mole fractions, we can calculate the partial pressures of helium and hydrogen. [Pg.84]

We have encountered the early nineteenth-century English chemist John Dalton before in the discussion to his development of the theory of atoms. Dalton also worked on the properties of gases. [Pg.233]

In a mixture of gases, the partial pressure of any one gas is the pressure that gas alone would exert if the other gases were removed (and volume and temperature were kept constant). Chemists had already noticed that the volume of liquids is not additive. For example, if 100 mL of one liquid is mixed with 100 mL of another liquid, the total volume is not exactly 200 mL—the total usually is a little less or a little more than 200 mL. Therefore, it was not clear that the pressure of two gases in a mixture should be additive. It was Dalton who argued that they are. [Pg.233]

Dalton s law of partial pressures states that The total pressure of a mixture of gases equals the sum of the partial pressures. It may sound simple to us today, but remember that Dalton lived before the ideal gas law or the kinetic theory of gases had been formulated. [Pg.233]

A pressure gauge only indicates total pressure, not the partial pressure due to each gas in a mixture. However, we can use the ideal gas law in the form P = to calculate each partial pressure. If only one gas is present, n equals the number of moles of that gas (found by dividing the mass of the gas by the molecular weight of the gas). By the kinetic theory of gases, the pressure a gas exerts is independent of the identity of the gas. All that matters is the number of particles of that gas that are present. In a mixture of gases, we know the volume and temperature. Therefore, if we know the mass of the various gases that have been mixed together, we can likewise calculate the number of moles of each gas present. Then, the partial pressure of each gas is just the number of moles of that gas times [Pg.234]

Note that when we add all the partial pressures together, all of the n s will add together to give the total number of moles of gases present. Thus, the sum of all of the individual partial pressures equals the total gas pressure that would be measured on a pressure gauge— Dalton s law of partial pressures. [Pg.234]

When two or more gaseous substances are placed in a container, each gas behaves as though it occupies the container alone. For example, if we place 1.00 mole of N2 gas in a 5.00-L container at 0°C, it exerts a pressure of [Pg.434]

If we then add a mole of another gas, such as O2, the pressure exerted by N2 does not change. It remains at 4.48 atm. The O2 gas exerts its own pressure, also 4.48 atm. Neither gas is affected by the presence of the other. In a mixture of gases, the pressure exerted by each gas is known as the partial pressure fPj) of the gas. We use subscripts to denote partial pressures  [Pg.434]

Sample Problem 11.11 shows how to apply Dalton s law of partial pressures. [Pg.435]

00-L vessel contains 0.215 mole of N2 gas and 0.0118 mole of H2 gas at 25.5 C. Determine the partial pressure of each component and the total pressure in the vessel. [Pg.435]

Studies of gaseous mixtures show that each component behaves independently of the others. In other words, a given amount of oxygen exerts the same pressure in a 1.0-L vessel whether it is alone or in the presence of nitrogen (as in the air) or helium. [Pg.464]

Among the first scientists to study mixtures of gases was John Dalton. In 1803 Dalton summarized his observations in this statement  [Pg.464]

The partial pressure of a gas is the pressure that the gas would exert if it were alone in the container. Dalton s law of partial pressures can be expressed as follows for a mixture containing three gases  [Pg.464]

So far, we ve limited our discussion to samples containing a single gas. Quite often, however, you are confronted with mixtures of gases (e.g., air). In 1801, John Dalton determined a relationship between gases in a mixture that is now referred to as Dalton s law ofpartial pressures. What he discovered is that the total pressure of a mixture of gases is equal to the sum of the partial pressures that each gas would exert if it were present alone. Expressed mathematically, this means that  [Pg.159]

While it may be obvious to you, it is worth stating that the total number of moles of gas in the sample is also equal to the sum of the number of moles of each gas in the sample  [Pg.159]

From this expression, it is possible to determine what percentage of a mixture is accounted for by a given substance. This is done by determining a quantity known as the mole fraction, which is defined as XA (where A is a variable that represents a gas in the mixture)  [Pg.159]

Equation 8.12 is useful because it allows us to determine the partial pressure of a gas if we know the total pressure and the amount present. The partial pressure of the gas will be proportional to the mole fraction of the gas in the mixture. This can be expressed as Equation 8.13  [Pg.159]

Finally, there is one more aspect of partial pressures that must be included. Most of the partial pressure problems that appear on the AP test involve gases that have been collected over a liquid. (In other words, they have been collected by displacement of the liquid, usually water.) The significance of this is that in the container, along with the collected gas, is vapor from the liquid, so the pressure in the collection vessel is the sum of the pressure of the gas and the vapor. Since we know that the total pressure in the container is equal to the sums of [Pg.159]

Assuming that each gas behaves ideally, the partial pressure of each gas can be calculated from the ideal gas law  [Pg.199]

The partial pressure of each gas in a mixture of gases in a container depends on the number of moies of that gas. The totai pressure is the sum of the partiai pressures and depends on the totai moies of gas particies present, no matter what they are. Note that the voiume remains constant. [Pg.199]

Copyright 2010 Cengage Learning, Inc. All Rights Reserved. May not be copied, scanned, or duplicated, in whole or in part. [Pg.199]

This important observation indicates some fundamental characteristics of an ideal gas. The fact that the pressure exerted by an ideal gas is not affected by the identity (composition) of the gas particles reveals two things about ideal gases (1) the volume of the individual gas particle must not be important, and (2) the forces among the particles must not be important. If these factors were important, the pressure exerted by the gas would depend on the nature of the individual particles. These observations will strongly influence the model that we will eventually construct to explain ideal gas behavior. [Pg.200]

One curious physical phenomenon associated with gases is the fact that when there is a mixture of gases in a given volume they behave independentiy so that their pressures are additive. In fact this raises the issue of what we mean by pressure. Common sense may lead us to expect that volumes are additive as indeed they are for macroscopic objects such as bricks. Thus, it is somewhat thought provoking that several gases can be easily confined in the same volume. This same sort of question also arises for mixtures of liquids to a much less extent as discussed later in Chapter 6. These considerations go to the very heart of the concept of the size of atoms and molecules and how much space is between them in a liquid or gas. As we will soon see, the space between gas molecules is about 100 times their size at 1 atm so there is plenty of space for other molecules. In addition, it will soon become evident that pressure is (force/area) caused by many collisions of gas molecules with the wall of the container. Cavendish in 1781 and Dalton in 1810 contributed to the concept now known as Dalton s law.  [Pg.11]

The most common use of Dalton s law is when gases are measured over water, that is, when a pressure is measured in the presence of moisture, which produces a partial pressure of water vapor as a gas, which in turn contributes a small pressure to the total pressure. This can occur when a reaction produces a gas and the gas is trapped in a container inverted over water. Tables of the vapor pressure of water are readily available in handbooks. Water is often in natural settings where gas pressure is measured in the presence of dew or a layer of water as may occur in wet forensic samples. In the distant past chemists often isolated gases as the product of a reaction and allowed the gas to bubble through a water trap, thereby introducing water vapor pressure into the total pressure. [Pg.11]

By Dalton s law of partial pressures the total pressure of 750 mmHg of the gas trapped over the water is the sum of the pressure of the water vapor and that of the N2 so we have [Pg.12]

Then we can calculate the moles of N2 from the ideal gas equation. [Pg.12]


Dalton s law of partial pressures The total pressure (P) exerted by a mixture of gases is equal to the sum of the partial pressures (p) of the components of the gas mixture. The partial pressure is defined as the pressure the gas would exert if it was contained in the same volume as that occupied by the mixture. [Pg.125]

Steam Distillation. Distillation of a Pair of Immiscible Liquids. Steam distillation is a method for the isolation and purification of substances. It is applicable to liquids which are usually regarded as completely immiscible or to liquids which are miscible to only a very limited extent. In the following discussion it will be assumed that the liquids are completely immiscible. The saturated vapours of such completely immiscible liquids follow Dalton s law of partial pressures (1801), which may be stated when two or more gases or vapoms which do not react chemically with one another are mixed at constant temperature each gas exerts the same pressure as if it alone were present and that... [Pg.12]

The Driving Force for Mass Transfer. The rate of mass transfer increases as the driving force, (7 — (7, is increased. can be enhanced as follows. From Dalton s law of partial pressures... [Pg.333]

When kc and K g values are reported in units (SI) of kmoL/[(s m") (kPa)], one must be careful in converting them to a mole-fracdion basis to multiply by the total pressure actually employed in the original experiments and not by the total pressure or the system to Be designed. This conversion is valid for systems in which Dalton s law of partial pressures p = ypr) is valid. [Pg.602]

Dalton S Law of Partial Pressures. The total pressure (P) of a gaseous mixture equals the sum of the partial pressures of its components. By definition, the partial pressure of any component gas is the hypothetical pressure it would exert by occupying the entire volume (V) of the mixture at the same temperature (T). That is,... [Pg.339]

Dalton s Law of partial pressures considers a mixture of two or more gases, and states that the total pressure of the mixture is equal to the sum of the individual pressures, if each gas separately occupied the space. [Pg.5]

It is almost independent of the presence of indifferent gases in the vapour-space (Law of Partial Pressures). [Pg.171]

This is nothing else than the well-known Law of Mixed Gases, or Law of Partial Pressures, discovered experimentally by John Dalton in 1801, and expressed by him in the somewhat vague... [Pg.265]

It was also found experimentally that two solutes were distributed between a pair of solvents as if each were present. alone. (This is analogous to Dalton s law of partial pressures.)... [Pg.313]

If we assume that Dalton s law of partial pressure holds in the vapor phase, it is easy to show that >2 is related to the total pressure, p, by the equation... [Pg.406]

Dalton s law of partial pressure 264, 406 Davies, C. A. 449, 456, 507 Debye heat capacity equation for solids 572-80, 651-4... [Pg.656]

Dalton summarized his observations in terms of the partial pressure of each gas, the pressure that the gas would exert if it occupied the container alone. In our example, the partial pressures of oxygen and nitrogen in the mixture are 0.60 atm and 0.40 atm, respectively, because those are the pressures that the gases exert when each one is in the container alone. Dalton then described the behavior of gaseous mixtures by his law of partial pressures ... [Pg.277]

This is Dalton s law of partial pressures. To obtain a total pressure, simply add the contributions from all gases present Ptotal Pi + P2 + P3 +------------ Pi... [Pg.314]

Gaseous solutions are easy to prepare and easy to describe. The atoms or molecules of a gas move about freely. When additional gases are added to a gaseous solvent, each component behaves independently of the others. Unless a chemical reaction occurs, the ideal gas equation and Dalton s law of partial pressures describe the behavior of gaseous solutions at and below atmospheric pressure (see Chapter 5). [Pg.829]

The water vapor mixes with any other gas(es) present, and the mixture is governed by Dalton s law of partial pressures, just like any other gas mixture. [Pg.193]

Dalton s Law of Partial Pressures states that Ptotai = Px + P2 + P2 +. .. [Pg.185]


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