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A tank in a room at \(19^{\circ} \mathrm{C}\) is initially open to the atmosphere on a day when the barometric pressure is 102 kPa. A block of dry ice (solid \(\mathrm{CO}_{2}\) ) with a mass of \(15.7 \mathrm{kg}\) is dropped into the tank, which is then sealed. The reading on the tank pressure gauge initially rises very quickly, then much more slowly, eventually reaching a value of 3.27 MPa. Assume \(T_{\text {final }}=19^{\circ} \mathrm{C}\) (a) How many moles of air were in the tank initially? Neglect the volume occupied by \(\mathrm{CO}_{2}\) in the solid state, and assume that a negligible amount of \(\mathrm{CO}_{2}\) escapes prior to the sealing of the tank. (b) Estimate the percentage error made by neglecting the volume of the block of dry ice placed in the tank. (The specific gravity of solid carbon dioxide is approximately 1.56 .) (c) What is the final density (g/L) of the gas in the tank? (d) Explain the observed variation of pressure with time. More specifically, what is happening in the tank during the initial rapid pressure increase and during the later slow pressure increase?

Short Answer

Expert verified
(a) The number of moles of air in the tank initially can be found using the ideal gas law, considering the given conditions. (b) The percentage error made by neglecting the volume of CO鈧 is small and can be calculated from the volume of CO鈧 and the total tank volume. (c) The final density of the gas in the tank can be found using the total moles of gas and the volume of the tank. (d) The initial rapid pressure increase is due to the sublimation of CO鈧, while the later slow increase is the result of thermal expansion due to the room temperature.

Step by step solution

01

Calculating initial moles of air in the tank

We can use the ideal gas equation \( P V= n R T \) to find the initial moles of air in the tank. First, convert the pressure P (102 kPa) into Pa by multiplying by 1,000; convert the temperature T (19掳C) into Kelvin by adding 273.15. Considering the initial volume V of the tank, we can rearrange the equation to \( n_{air} = \frac{PV}{RT} \) where R (8.314 J/ mol路K) is the gas constant.
02

Calculating the moles and volume of CO鈧

Calculate the moles of CO鈧 using the mass and the molar mass of CO鈧 (44 g/mol): \( n_{CO2} = \frac{mass_{CO2}}{MolarMass_{CO2}} \). The volume of CO鈧 can be estimated using the specific gravity and the mass of CO鈧: \( V_{CO2} = \frac{mass_{CO2}}{density_{CO2}} \) where density of CO鈧 is obtained by multiplying the specific gravity by the density of water (1,000 kg/m鲁). The percentage error due to neglecting this volume is then \( \frac{V_{CO2}}{V_{tank}} * 100\% \)
03

Calculating the final density of the gas in the tank

Total mole of gas in the tank is given by \( n_{total} = n_{air} + n_{CO2} \). Then, applying the ideal gas law again in the final situation and solving for density (蟻), we find \( 蟻 = \frac{n_{total} * MolarMass_{air}}{V_{tank}} \) where MolarMass_air is the molar mass of air (28.97 g/mol).
04

Interpreting the variation of pressure with time

The initial rapid pressure increase in the tank is due to the sublimation of solid CO鈧 into gas, increasing the number of gas particles and hence the pressure. The later slow pressure increase is due to the warm room temperature causing further expansion of the gas particles, thus gradually increasing the pressure.

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Key Concepts

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

Pressure Variation
In the exercise, we observe two distinct phases regarding the change in pressure inside the tank. The initial rapid pressure increase occurs when the dry ice, which is solid carbon dioxide (CO鈧), is introduced into the tank and begins to sublimate.
This means that the CO鈧 transitions directly from a solid state to a gaseous state, significantly adding to the number of gas particles in the tank and consequently leading to a quick rise in pressure.

After the initial burst of pressure, the rate of increase slows down. This is because, once the tank is sealed, the additional pressure changes depend more on temperature than on the sublimation process.
The room temperature, which remains consistent, causes a gradual expansion of the gas particles.
Gas particles move faster and further apart as their kinetic energy increases with temperature, leading to a slow but steady increase in pressure over time.

Key points to understand pressure variation include:
  • The role of sublimation in rapidly increasing pressure by adding gas particles.
  • The effect of temperature on slowly increasing pressure by expanding gas particles.
  • Understanding pressure dynamics is essential for applications involving enclosed environments where temperature and phase changes occur.
Moles Calculation
The Ideal Gas Law, represented by the formula \( PV = nRT \), is a powerful tool for determining the number of moles of a gas.
In this exercise, to find the initial moles of air in the tank, we convert given atmospheric pressure from kilopascals to pascals and temperature from Celsius to Kelvin.
The number of moles \( n \) is then given by rearranging the Ideal Gas Law to \( n = \frac{PV}{RT} \).

The gas constant \( R \) is a universal value that makes these calculations consistent, typically using \( 8.314 \, \text{J/mol}\cdot\text{K} \).
This relationship shows the direct proportionality between the amount of gas (in moles) and the product of pressure and volume over the temperature.

Mole calculations help us:
  • Predict how much product will form in a chemical reaction.
  • Understand the relationship between pressure, volume, and temperature in a given setting.
  • Ensure accuracy in scientific measurements and industrial applications involving gases.
Gas Density
Gas density refers to the mass of gas per unit volume and is a critical parameter in understanding how gases will behave under different conditions.
In this exercise, after determining the total number of gas moles in the tank, we apply the Ideal Gas Law to ascertain the gas density.
The final density is calculated as \( \rho = \frac{n_{total} \times \text{MolarMass}_{\text{air}}}{V_{\text{tank}}} \), where the molar mass of air is approximately \( 28.97 \, \text{g/mol} \).

This formula highlights that density is dependent on both the total amount of gas added and its molar mass.
Gas density is directly proportional to pressure and inversely proportional to volume and temperature when we consider a closed system.

Understanding gas density is crucial because it affects:
  • The buoyancy behavior in different fluids, impacting things like balloon flights and airborne toxin dispersion.
  • The sound speed in gases since denser gases conduct sound more slowly.
  • Calculations needed in thermodynamics and fluid mechanics for designing efficient systems.
CO2 Sublimation
Sublimation is the process in which a solid transitions directly into a gas without passing through a liquid phase.
One of the most well-known sublimating substances is Carbon Dioxide (CO鈧) - commonly referred to as dry ice.
When dry ice is placed into an open container at room temperature, it will sublimate entirely into gaseous CO鈧.

During sublimation, there is a rapid increase in the number of molecules in the gaseous state, translating into an increase in pressure inside a confined space.
For CO鈧, sublimation occurs at temperatures below its triple point, where the solid ice skips the liquid state and directly turns into a gas.

Here is why understanding CO鈧 sublimation is important:
  • It helps in refrigeration processes, where cooling is achieved by removing heat via the sublimating gas.
  • It requires caution in handling because sublimated CO鈧 can cause pressure buildup in sealed containers.
  • It's useful in industries where rapid transitions from solid to gas are necessary, such as cleaning objects without residue.

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Most popular questions from this chapter

Magnesium sulfate has a number of uses, some of which are related to the ability of the anhydrate form to remove water from air and others based on the high solubility of the heptahydrate \(\left(\mathrm{MgSO}_{4} \cdot 7 \mathrm{H}_{2} \mathrm{O}\right)\) form, also known as Epsom salt. The densities of the anhydrate and heptahydrate crystalline forms are 2.66 and \(1.68 \mathrm{g} / \mathrm{mL},\) respectively. Suppose you wish to form a 20.0 wt\% \(\mathrm{MgSO}_{4}\) aqueous solution by simply pouring crystals of one of the forms into a tank of water while the temperature is held constant at \(30^{\circ} \mathrm{C}\). The specific gravity of the 20.0 wt\% solution at \(30^{\circ} \mathrm{C}\) is \(1.22 .\) Answer the following questions for both forms of the \(\mathrm{MgSO}_{4}\) crystals: (a) What volume of water should be in the tank before crystals are added if the final product is to be 1000 kg of the 20 wt\% solution? (b) Suppose the tank diameter is \(0.30 \mathrm{m}\). What is the height of liquid in the tank before the crystals are added? (c) What is the height of the water in the tank after addition of the crystals but before they begin to dissolve? (d) What is the height of liquid in the tank after all the MgSO \(_{4}\) has dissolved?

The concentration of oxygen in a 5000 -liter tank containing air at 1 atm is to be reduced by pressure purging prior to charging a fuel into the tank. The tank is charged with nitrogen up to a high pressure and then vented back down to atmospheric pressure. The process is repeated as many times as required to bring the oxygen concentration below 10 ppm (i.c., to bring the mole fraction of \(\mathrm{O}_{2}\) below \(10.0 \times 10^{-6}\) ). Assume that the temperature is \(25^{\circ} \mathrm{C}\) at the beginning and end of each charging cycle. When doing \(P V T\) calculations in Parts (b) and (c), use the generalized compressibility chart if possible for the fully charged tank and assume that the tank contains pure nitrogen. (a) Speculate on why the tank is being purged. (b) Estimate the gauge pressure (atm) to which the tank must be charged if the purge is to be done in one charge-vent cycle. Then estimate the mass of nitrogen (kg) used in the process. (For this part, if you can't find the tank condition on the compressibility chart, assume ideal-gas behavior and state whether the resulting estimate of the pressure is too high or too low.) (c) Suppose nitrogen at 700 kPa gauge is used for the charging. Calculate the number of charge-vent cycles required and the total mass of nitrogen used. (d) Use your results to explain why multiple cycles at a lower gas pressure are preferable to a single cycle. What is a probable disadvantage of multiple cycles?

Ethane at \(25^{\circ} \mathrm{C}\) and 1.1 atm (abs) flowing at a rate of \(100 \mathrm{mol} / \mathrm{s}\) is burned with \(20 \%\) excess oxygen at \(175^{\circ} \mathrm{C}\) and 1.1 atm \((\text { abs }) .\) The combustion products leave the furnace at \(800^{\circ} \mathrm{C}\) and 1 atm. (a) What is the volumetric flow rate of oxygen (L/s) fed to the furnace? (b) What should the volumetric flow rate of the combustion products be? State all assumptions you make. (c) The volumetric flow rate of the combustion products is measured and found to be different from the value calculated in Part (b). Assuming that no mistakes were made in the calculation, what could be going on that could lead to the discrepancy? Consider assumptions made in the calculations and things that can go wrong in a real system.

A balloon \(20 \mathrm{m}\) in diameter is filled with helium at a gauge pressure of 2.0 atm. A man is standing in a basket suspended from the bottom of the balloon. A restraining cable attached to the basket kecps the balloon from rising. The balloon (not including the gas it contains), the basket, and the man have a combined mass of \(150 \mathrm{kg}\). The temperature is \(24^{\circ} \mathrm{C}\) that day, and the barometer reads \(760 \mathrm{mm} \mathrm{Hg}\) (a) Calculate the mass (kg) and weight (N) of the helium in the balloon. (b) How much force is exerted on the balloon by the restraining cable? (Recall: The buoyant force on a submerged object equals the weight of the fluid- -in this case, the air- -displaced by the object. Neglect the volume of the basket and its contents.) (c) Calculate the initial acceleration of the balloon when the restraining cable is released. (d) Why does the balloon eventually stop rising? What would you need to know to calculate the altitude at which it stops? (e) Suppose at its point of suspension in midair the balloon is heated, raising the temperature of the helium. What happens and why?

Spray drying is a process in which a liquid containing dissolved or suspended solids is injected into a chamber through a spray nozzle or centrifugal disk atomizer. The resulting mist is contacted with hot air, which evaporates most or all of the liquid, leaving the dried solids to fall to a conveyor belt at the bottom of the chamber. Powdered milk is produced in a spray dryer \(6 \mathrm{m}\) in diameter by \(6 \mathrm{m}\) high. Air enters at \(167^{\circ} \mathrm{C}\) and \(-40 \mathrm{cm} \mathrm{H}_{2} \mathrm{O}\). The milk fed to the atomizer contains \(70 \%\) water by mass, all of which evaporates. The outlet gas contains 12 mole \(\%\) water and leaves the chamber at \(83^{\circ} \mathrm{C}\) and \(1 \mathrm{atm}\) (absolute) at a rate of \(311 \mathrm{m}^{3} / \mathrm{min}\). (a) Calculate the production rate of dried milk and the volumetric flow rate of the inlet air. Estimate the upward velocity of air (m/s) at the bottom of the dryer. (b) Engineers often face the challenge of what to do to a process when demand for a product increases (or decreases). Suppose in the present case production must be doubled. (i) Why is it unlikely that the flow rates of feed and air can simply be increased to achieve the new production rate? (ii) An obvious option is to buy another dryer like the existing one and operate the two in parallel. Give two advantages and two disadvantages of this option. (iii) Still another possibility is to buy a larger dryer to replace the original unit. Give two advantages and two disadvantages of doing so. Estimate the approximate dimensions of the larger unit.

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