/*! 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 89 Oxygen therapy uses various devi... [FREE SOLUTION] | 91Ó°ÊÓ

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Oxygen therapy uses various devices to provide oxygen to patients having difficulty getting sufficient amounts from air through normal breathing. Among the devices is a nasal cannula, which transports oxygen through small plastic tubes from a supply tank to prongs placed in the nostril. Consider a specific configuration in which the supply tank, whose volume is \(6.0 \mathrm{ft}^{3},\) is filled to a pressure of 2100 psig at a temperature of \(85^{\circ} \mathrm{F}\). The paticnt is in an environment where the ambicnt temperature is \(40^{\circ} \mathrm{F}\). When the cannula is put into use, the pressure in the tank begins to decrease as oxygen flows at \(10-15 \mathrm{L} / \mathrm{min}\) through a tube and the cannula into the nostrils. (a) Estimate the original mass of oxygen in the tank using the compressibility-factor equation of state. (b) What is the initial pressure when the temperature is 40 \(^{\circ} \mathrm{F} ?\) How much oxygen remains in the tank when application of the ideal-gas equation of state produces a result that is within \(3 \%\) of that predicted by the compressibility-factor equation of state (i.e., when \(0.97 \leq z \leq 1.03\) )? (c) How long will it take for the gauge on the tank to read 50 psig, assuming an average flow rate of \(12.5 \mathrm{L} / \mathrm{min} ?\)

Short Answer

Expert verified
From the calculations, the original mass of the oxygen in the tank is approximately 2.95 lb. The initial pressure at 40F is approximately 1963 psig. The time it will take for the gauge to read 50 psig is around 167 minutes.

Step by step solution

01

Calculate the Original Mass of Oxygen

To find the original mass, one can use the compressibility factor equation of state, given by \(PV = ZnRT\). Here, \(P\) is the pressure, \(V\) is the volume, \(Z\) is the compressibility factor, \(n\) is the number of moles, \(R\) is the gas constant, and \(T\) is the temperature. Since the mass (\(m\)) can be calculated by \(m = nM\), where \(M\) is the molar mass, rearranging the equation to solve for \(m\) gives \(m = \frac{PVM}{ZRT}\). Plugging in the provided values (converting units as necessary): \(P = 2100\) psig, \(V = 6.0\) ft\(^3\), \(Z = 1\) (for Oxygen at these conditions), \(R = 0.7302\) atm.ft\(^3\).(lb.mol)\(^{-1}\).K\(^{-1}\), \(T = 85\) F = 532.67 Rankine, and \(M = 32\) g/mol = 32 lb/lb.mol, one can solve for \(m\).
02

Calculate the Initial Pressure at 40F

The ideal gas equation of state is given by \(PV = nRT\). Here, the task is to find the initial pressure (\(P\)). Rearranging for \(P\), we get \(P = \frac{nRT}{V}\). Here \(n\), the number of moles, can be calculated from mass and molar mass. With \(m = 2.95\) lb, \(M = 32\) lb/lb.mol: \(n = \frac{m}{M}\). Substituting this into the equation for \(P\) gives \(P = \frac{RTm}{VM}\), substituting the values (converting the temperature to Rankine): \(R = 0.7302\) atm.ft\(^3\).(lb.mol)\(^{-1}\).K\(^{-1}\), \(T = 40\) F = 491.67 Rankine, \(V = 6.0\) ft\(^3\), \(m = 2.95\) lb, and \(M = 32\) lb/lb.mol, one can solve for \(P\).
03

Calculate Time Until Gauge Reads 50 psig

We'll use the same principle as in step 2, rearranging the ideal gas equation to solve for \(n = \frac{PV}{RT}\). Substituting \(P = 50\) psig, \(V = 6.0\) ft\(^3\), \(R = 0.7302\) atm.ft\(^3\).(lb.mol)\(^{-1}\).K\(^{-1}\), and \(T = 491.67\) Rankine, to solve for \(n\). Then, calculate the mass of oxygen \(m = nM\), with \(M = 32\) lb/lb.mol. Use the volumetric flow rate given (\(12.5\) L/min) to calculate flow rate in terms of mass (\(F_m\)), knowing that \(1\) L oxygen weighs \(1.429\) g. Finally, use \(t = \frac{m}{F_m}\) to solve for time \(t\).

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Key Concepts

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

Understanding the Compressibility-Factor Equation
When studying the characteristics of gases under various conditions, the compressibility-factor equation is a crucial concept. It's a more generalized form of the ideal gas law, accounting for deviations from ideal behavior due to interactions between gas molecules and the volume they occupy. The compressibility factor, denoted as 'Z', is a measure of how much the behavior of a real gas deviates from an ideal gas; it is the ratio of the actual volume to the ideal volume at a given pressure and temperature.

In the given exercise, the compressibility-factor equation is used to estimate the original mass of oxygen in a tank. This involves understanding the relationship between pressure (P), volume (V), the number of moles (n), the gas constant (R), and temperature (T). When Z is equal to 1, a gas behaves ideally, but this is rarely the case for real gases under non-ideal conditions such as high pressure or low temperature. By manipulating the equation and incorporating the molar mass (M), we can solve for the mass of the gas.

The ideal compressibility-factor equation, which incorporates the Z factor, is expressed as:
\[ PV = ZnRT \]
For our oxygen therapy tank scenario, the factors are plugged into this equation to find the mass of oxygen present initially, considering the conditions stated. Real gases, like oxygen, often use a Z value close to 1 under standard conditions, but this can shift significantly under the high pressures found in compressed gas tanks.
The Ideal Gas Law in Practice
The ideal gas law is fundamental in the understanding of gas behavior under various conditions. It's an approximation that describes how gases expand, contract, and exert pressure. The law is usually expressed as:
\[ PV = nRT \]
where P stands for pressure, V for volume, n for the number of moles of the gas, R for the universal gas constant, and T for temperature in Kelvin. The ideal gas law assumes that gas molecules have negligible volume and experience no intermolecular forces.

In practical applications like oxygen delivery systems for therapy, the ideal gas law is useful to predict behaviors like the change in a gas's pressure as the temperature drops or the amount of time before a tank depletes at a consistent flow rate. However, the law has its limitations and does not always account for real gas behaviors, especially at high pressures or low temperatures. In the exercise, you can see the comparison between the compressibility-factor equation and the ideal gas law by determining the state of the oxygen under different temperatures and pressures.

Applying the ideal gas law to the exercise's part (b), we can calculate the change in pressure as the temperature of the oxygen adjusts from the storage condition to the ambient temperature of the patient's environment. This is crucial for systems like nasal cannulas, where controlled and consistent oxygen supply is necessary for patient well-being.
Oxygen Therapy Delivery Systems
Oxygen therapy is critical in medical treatments where patients cannot intake enough oxygen through natural breathing. This therapy involves devices, such as nasal cannulas, which deliver oxygen directly to the patient's nostrils. Understanding the operation of these devices is essential for healthcare professionals to ensure proper dosage and monitoring.

A nasal cannula is a simple, comfortable device consisting of a lightweight tube with two prongs that are inserted into the nostrils. It's connected to an oxygen supply tank, and the flow rate can be adjusted according to the patient's requirements. The exercise demonstrates how to calculate the duration of oxygen supply provided by such a tank, crucial for making sure patients receive uninterrupted therapy.

The calculations considering the ideal gas law assist healthcare providers to determine how long the tank will last (as explored in part (c) of the exercise) at a given flow rate. This kind of prediction is vital for managing the resources in healthcare settings, ensuring that patients have a continuous supply of oxygen and that tanks are replaced or refilled timely. Moreover, understanding the properties of oxygen and the physical laws governing its delivery allows for the safe and efficient use of therapy systems.

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Most popular questions from this chapter

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