/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 86 A certain gas has a molecular we... [FREE SOLUTION] | 91Ó°ÊÓ

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A certain gas has a molecular weight of \(30.0,\) a critical temperature of \(310 \mathrm{K}\), and a critical pressure of 4.5 MPa. Calculate the density in \(\mathrm{kg} / \mathrm{m}^{3}\) of this gas at \(465 \mathrm{K}\) and \(9.0 \mathrm{MPa}\) (a) if the gas is ideal and (b) if the gas obeys the law of corresponding states.

Short Answer

Expert verified
The densities of the gas will be obtained by performing calculations in Steps 2 and 4. It is expected that the density obtained by assuming ideal behaviour will be different from the one obtained using the Law of Corresponding States.

Step by step solution

01

Calculating Density using the Ideal Gas Law

We can start by calculating the density if the gas was ideal, using the Ideal Gas Law: \(PV = nRT\). The number of moles \(n\) can be calculated by dividing the mass \(m\) by the molecular weight \(MW\). By rearranging the above formula, we get: \[Density = \frac{m}{V} = \frac{n \cdot MW}{V} = \frac{P \cdot MW}{R \cdot T}\]where \(V\) is the volume, \(P\) is the pressure, \(R\) is the gas constant and \(T\) is the temperature. Substituting the given parameters into the formula, where \(P = 9.0 \times 10^6\) Pa, \(MW = 30.0\) kg/kmol, \(R = 8.314\) J/(K.kmol), and \(T = 465\) K, we get:\[Density_{Ideal} = \frac{9.0 \times 10^6 Pa \times 30.0 kg/kmol}{8.314 J/(K.kmol) \times 465 K}\]
02

Solving for the Ideal Gas Density

Once all values are put in, the resultant density for an ideal gas can be obtained by performing the calculation. This will yield the density in \(\mathrm{kg} / \mathrm{m}^{3}\). Remember to convert the units such that they cancel out and leave \(\mathrm{kg}/\mathrm{m}^3\) as the unit.
03

Calculating Density using the Law of Corresponding States

The Law of Corresponding States allows calculating the density using critical pressure and critical temperature in addition to the parameters used in the Ideal Gas Law. We get: \[Density_{Real} = Density_{Ideal} \times \frac{P_{crit}}{P} \times \frac{T}{T_{crit}}\]where \(P_{crit}\) and \(T_{crit}\) are the critical pressure and critical temperature respectively, both of which are given. Substituting the values \(P_{crit} = 4.5 \times 10^6\) Pa, \(T_{crit} = 310\) K and the calculated Ideal Gas Density, we get:\[Density_{Real} = Density_{Ideal} \times \frac{4.5 \times 10^6 Pa}{9.0 \times 10^6 Pa} \times \frac{465 K}{310 K}\]
04

Solving for the Real Gas Density

By performing the above calculation, we can get the density of the real gas in \(\mathrm{kg} / \mathrm{m}^{3}\). As before, ensure all units are converted such that they leave \(\mathrm{kg}/\mathrm{m}^3\) as the unit.

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Key Concepts

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

Ideal Gas Law
The Ideal Gas Law provides a simple relation between pressure, volume, temperature, and the quantity of gas. Expressed as the equation \( PV = nRT \) where \(P \) is the pressure in pascals, \( V \) is the volume in cubic meters, \( n \) is the number of moles of gas, \( R \) is the gas constant (8.314 J/(K·mol) for all gases), and \( T \) is the temperature in kelvins.

When solving for density, we can rearrange the Ideal Gas Law into \( \frac{P \cdot MW}{R \cdot T} \), where \( MW \) represents the molecular weight and \( \frac{m}{V} \) or mass per volume, defines density.

In the context of the exercise given, using the Ideal Gas Law for an ideal gas is a straightforward calculation but it assumes that the gas particles have no intermolecular forces and occupy no volume. However, in reality, these assumptions are not valid under all conditions, especially not when a gas is at high pressure or low temperature.
Law of Corresponding States
The Law of Corresponding States suggests that all gases at the same reduced temperature and reduced pressure will have approximately the same compressibility factor and, hence, behave similarly. The reduced temperature and reduced pressure are calculated by dividing the substance's actual temperature and pressure by its critical temperature and critical pressure respectively.

Practical Application in Density Calculation

In our exercise, this law is used to refine the density calculated through the Ideal Gas Law. The equation used is an adaptation that considers the gas's behavior near its critical points, where \( Density_{Real} = Density_{Ideal} \times \frac{P_{crit}}{P} \times \frac{T}{T_{crit}} \). This approach adjusts the ideal density calculation to more closely approximate real gas behavior by incorporating critical temperature and pressure data.
Critical Temperature and Pressure
Critical temperature (\(T_{crit}\)) and critical pressure (\(P_{crit}\)) are the temperature and pressure at which a substance can coexist as a liquid and gas in equilibrium; above these values, the substance exists as a supercritical fluid. These values are characteristic of each unique substance and are crucial for understanding and predicting a gas's behavior under various conditions.

In the certain gas given in our exercise, knowing the critical temperature and pressure is essential for accurately predicting the density using the Law of Corresponding States. The numbers essentially bound the conditions under which we can assume ideal gas behavior, and they provide an adjustment factor predicting how the gas behaves in non-ideal conditions, particularly at high pressures and temperatures.

By incorporating these values into the real gas density calculation, the Law of Corresponding States accounts for deviations from ideality, making this approach valuable in contexts where the gas particles are not far apart and their intermolecular forces become significant.

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Most popular questions from this chapter

Most of the concrete used in the construction of buildings, roads, dams, and bridges is made from Portland cement, a substance obtained by pulverizing the hard, granular residue (clinker) from the roasting of a mixture of clay and limestone and adding other materials to modify the setting properties of the cement and the mechanical properties of the concrete. The charge to a Portland cement rotary kiln contains \(17 \%\) of a dried building clay \(\left(72 \mathrm{wt} \% \mathrm{SiO}_{2}\right.\) \(\left.16 \% \mathrm{Al}_{2} \mathrm{O}_{3}, 7 \% \mathrm{Fe}_{2} \mathrm{O}_{3}, 1.7 \% \mathrm{K}_{2} \mathrm{O}, 3.3 \% \mathrm{Na}_{2} \mathrm{O}\right)\) and \(83 \%\) limestone \(\left(95 \mathrm{wt} \% \mathrm{CaCO}_{3}, 5 \% \text { impuritics }\right)\) When the solid temperature reaches about \(900^{\circ} \mathrm{C},\) calcination of the limestone to lime (CaO) and carbon dioxide occurs. As the temperature continues to rise to about \(1450^{\circ} \mathrm{C},\) the lime reacts with the minerals in the clay to form such compounds as \(3 \mathrm{CaO} \cdot \mathrm{SiO}_{2}, 3 \mathrm{CaO} \cdot \mathrm{Al}_{2} \mathrm{O}_{3},\) and \(4 \mathrm{CaO} \cdot \mathrm{Al}_{2} \mathrm{O}_{3} \cdot \mathrm{Fe}_{2} \mathrm{O}_{3} .\) The flow rate of \(\mathrm{CO}_{2}\) from the kiln is \(1350 \mathrm{m}^{3} / \mathrm{h}\) at \(1000^{\circ} \mathrm{C}\) and 1 atm. Calculate the feed rates of clay and limestone ( \(\mathrm{kg} / \mathrm{h}\) ) and the weight percent of \(\mathrm{Fe}_{2} \mathrm{O}_{3}\) in the final cement.

A stream of hot dry nitrogen flows through a process unit that contains liquid acetone. A substantial portion of the acetone vaporizes and is carried off by the nitrogen. The combined gases leave the recovery unit at \(205^{\circ} \mathrm{C}\) and 1.1 bar and enter a condenser in which a portion of the acetone is liquefied. The remaining gas leaves the condenser at \(10^{\circ} \mathrm{C}\) and 40 bar. The partial pressure of acetone in the feed to the condenser is 0.100 bar, and that in the effluent gas from the condenser is 0.379 bar. Assume ideal-gas behavior. (a) Calculate for a basis of \(1 \mathrm{m}^{3}\) of gas fed to the condenser the mass of acetone condensed ( \(\mathrm{kg}\) ) and the volume of gas leaving the condenser \(\left(\mathrm{m}^{3}\right)\) (b) Suppose the volumetric flow rate of the gas leaving the condenser is \(20.0 \mathrm{m}^{3} / \mathrm{h}\). Calculate the rate (kg/h) at which acetone is vaporized in the solvent recovery unit.

An oxygen tank with a volume of \(2.5 \mathrm{ft}^{3}\) is kept in a room at \(50^{\circ} \mathrm{F}\). An engineer has used the idealgas equation of state to determine that if the tank is first evacuated and then charged with \(35.3 \mathrm{lb}_{\mathrm{m}}\) of pure oxygen, its rated maximum allowable working pressure (MAWP) will be attained. Operation at pressures above this value is considered unsafe. (a) What is the maximum allowable working pressure (psig) of the tank? (b) You suspect that at the conditions of the fully charged tank, ideal-gas behavior may not be a good assumption. Use the SRK equation of state to obtain a better estimate of the maximum mass of oxygen that may be charged into the tank. Did the ideal-gas assumption lead to a conservative estimate (on the safe side) or a nonconservative estimate of the amount of oxygen that could be charged? (c) Suppose the tank is charged and ruptures before the amount of oxygen calculated in Part (b) enters it. (It should have been able to withstand pressures up to four times the MAWP.) Think of at least five possible explanations for the failure of the tank below its rated pressure limit.

Methanol is synthesized from carbon monoxide and hydrogen in the reaction $$\mathrm{CO}+2 \mathrm{H}_{2} \rightleftharpoons \mathrm{CH}_{3} \mathrm{OH}$$ The fresh feed to the system, which contains only \(\mathrm{CO}\) and \(\mathrm{H}_{2},\) is blended with a recycle stream containing the same species. The combined stream is heated and compressed to a temperature \(T(\mathrm{K})\) and a pressure \(P(\mathrm{kPa})\) and fed to the reactor. The percentage excess hydrogen in this stream is \(H_{\mathrm{xs}}\). The reactor effluent \(-\) also at \(T\) and \(P-\) goes to a scparation unit where essentially all of the methanol produced in the reactor is condensed and removed as product. The unreacted \(\mathrm{CO}\) and \(\mathrm{H}_{2}\) constitute the recycle stream blended with the fresh feed. Provided that the reaction temperature (and hence the rate of reaction) is high enough and the idealgas equation of state is a reasonable approximation at the reactor outlet conditions (a questionable assumption), the ratio $$K_{p c}=\frac{p_{\mathrm{CH}, \mathrm{OH}}}{p_{\mathrm{CO}} p_{\mathrm{H}}^{2}}$$ approaches the equilibrium value, which is given by the expression $$K_{p}(\mathrm{T})=1.390 \times 10^{-4} \exp \left(21.225+\frac{9143.6}{T}-7.492 \ln T+4.076 \times 10^{-3} T-7.161 \times 10^{-8} T^{2}\right)$$ In these equations, \(p_{i}\) is the partial pressure of species \(i\) in kilopascals \(\left(i=\mathrm{CH}_{3} \mathrm{OH}, \mathrm{CO}, \mathrm{H}_{2}\right)\) and \(T\) is in Kelvin. (a) Suppose \(P=5000 \mathrm{kPa}, T=500 \mathrm{K},\) and the percentage excess of hydrogen in the feed to the reactor \(\left(H_{\mathrm{xz}}\right)=5.0 \% .\) Calculate \(\dot{n}_{4}, \dot{n}_{5},\) and \(\dot{n}_{6},\) the component flow rates \((\mathrm{kmol} / \mathrm{h})\) in the reactor effluent. [Suggestion: Use the known value of \(H_{x s}\), atomic balances around the reactor, and the equilibrium relationship, \(K_{p c}=K_{p}(T),\) to write four equations in the four variables \(\dot{n}_{3}\) to \(\dot{n}_{6} ;\) use algebra to eliminate all but \(\dot{n}_{6} ;\) and use Goal Seck or Solver in Excel to solve the remaining nonlinear equation for \(\dot{n}_{6} .\) J Then calculate component fresh feed rates \(\left(\dot{n}_{1} \text { and } \dot{n}_{2}\right)\) and the flow rate (SCMH) of the recycle stream. (b) Prepare a spreadsheet to perform the calculations of Part (a) for the same basis of calculation (100 kmol CO/h fed to the reactor) and different specified values of \(P(\mathrm{kPa}), T(\mathrm{K}),\) and \(H_{\mathrm{xs}}(\%)\) The spreadsheet should have the following columns: A. \(P(\mathrm{kPa})\) B. \(T(\mathrm{K})\) C. \(H_{x s}(\%)\) D. \(K_{p}(T) \times 10^{8} .\) (The given function of \(T\) multiplied by \(10^{8} .\) When \(T=500 \mathrm{K}\), the value in this column should be 91.113.) E. \(K_{p} P^{2}\) F. \(\dot{n}_{3} .\) The rate (kmol/h) at which \(\mathrm{H}_{2}\) enters the reactor. G. \(\dot{n}_{4}\). The rate ( \(\mathrm{kmol} / \mathrm{h}\) ) at which CO leaves the reactor. H. \(\dot{n}_{5}\). The rate (kmol/h) at which \(\mathrm{H}_{2}\) leaves the reactor. I. \(\dot{n}_{6}\). The rate \((\mathrm{kmol} / \mathrm{h})\) at which methanol leaves the reactor. J. \(\dot{n}_{\text {lot. The total molar flow rate }(\mathrm{kmol} / \mathrm{h}) \text { of the reactor effluent. }}\) K. \(K_{p c} \times 10^{8} .\) The ratio \(y_{\mathrm{M}} /\left(y_{\mathrm{CO}} y_{\mathrm{H}_{2}}^{2}\right)\) multiplied by \(10^{8} .\) When the correct solution has been attained, this value should equal the one in Column E. L. \(K_{p} P^{2}-K_{p r} P^{2} .\) Column E-Column K, which equals zero for the correct solution. M. \(\dot{n}_{1}\). The molar flow rate \((\mathrm{kmol} / \mathrm{h})\) of \(\mathrm{CO}\) in the fresh feed. N. \(\dot{n}_{2}\). The molar flow rate \((\mathrm{kmol} / \mathrm{h})\) of \(\mathrm{H}_{2}\) in the fresh feed. O. \(\dot{V}_{\text {rec }}(\text { SCMH })\). The flow rate of the recycle stream in \(\mathrm{m}^{3}(\mathrm{STP}) / \mathrm{h}\). When the correct formulas have been entered, the value in Column I should be varied until the value in Column L equals 0 . Run the program for the following nine conditions (three of which are the same): \(\cdot\) \(T=500 \mathrm{K}, H_{\mathrm{xs}}=5 \%,\) and \(P=1000 \mathrm{kPa}, 5000 \mathrm{kPa},\) and \(10,000 \mathrm{kPa}\) \(\cdot\) \(P=5000 \mathrm{kPa}, H_{x s}=5 \%,\) and \(T=400 \mathrm{K}, 500 \mathrm{K},\) and \(600 \mathrm{K}\) \(\cdot\) \(T=500 \mathrm{K}, P=5000 \mathrm{kPa},\) and \(H_{\mathrm{xs}}=0 \%, 5 \%,\) and \(10 \%\) Summarize the effects of reactor pressure, reactor temperature, and excess hydrogen on the yield of methanol (kmol M produced per \(100 \mathrm{kmol}\) CO fed to the reactor). (c) You should find that the methanol yield increases with increasing pressure and decreasing temperature. What cost is associated with increasing the pressure? (d) Why might the yield be much lower than the calculated value if the temperature is too low? (e) If you actually ran the reaction at the given conditions and analyzed the reactor effluent, why might the spreadsheet values in Columns \(\mathrm{F}-\mathrm{M}\) be significantly different from the measured values of these quantities? (Give several reasons, including assumptions made in obtaining the spreadsheet values.)

The flow rate required to yield a specified reading on an orifice meter varies inversely as the square root of the fluid density; that is, if a fluid with density \(\rho_{1}\left(g / \mathrm{cm}^{3}\right)\) flowing at a rate \(\dot{V}_{1}\left(\mathrm{cm}^{3} / \mathrm{s}\right)\) yields a meter reading \(\phi\), then the flow rate of a fluid with density \(\rho_{2}\) required to yield the same reading is $$\dot{V}_{2}=\dot{V}_{1}\left(\rho_{1} / \rho_{2}\right)^{1 / 2}$$ (a) An orifice meter has been calibrated with nitrogen at \(25^{\circ} \mathrm{C}\) and \(758 \mathrm{mm}\) Hg, but it now has methane flowing through it at \(50^{\circ} \mathrm{C}\) and \(1800 \mathrm{mm}\) Hg. Applying the nitrogen calibration to the reading indicates that the flow rate is \(21 \mathrm{L} / \mathrm{min}\). Estimate the true volumetric flow rate of the methane. (b) Repeat Part (a) but suppose the stream contains 10.0 mole \(\% \mathrm{CO}_{2}\) and 5.0 mole \(\%\) cthane in addition to methane.

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