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A vessel of volume \(V_{0}\) contains an ideal gas at pressure \(p_{0}\) and temperature \(T\). Gas is continuously pumped out of this vessel at a constant volume-rate \(d V / d t=r\) keeping the temperature constant. The pressure of the gas being taken out equals the pressure inside the vessel. Find (a) the pressure of the gas as a function of time, (b) the time taken before half the original gas is pumped out.

Short Answer

Expert verified
(a) \( p(t) = p_0 - \frac{rRT}{V_0^2}t \); (b) \( t_{1/2} = \frac{V_0^2}{2rRT}p_0 \).

Step by step solution

01

Ideal Gas Law Application

We start by applying the ideal gas law, which is \( pV = nRT \). Given that the temperature \( T \) remains constant, we have \( pV = n_0RT \), where \( n_0 \) is the initial number of moles. Since \( n_0 \) and \( T \) are constants, initially \( p_0V_0 = n_0RT \). Let \( n(t) \) denote the amount of gas left at time \( t \). Then the pressure at time \( t \), \( p(t) \), is \( p(t)V_0 = n(t)RT \).
02

Express Rate of Change of Moles

The rate at which gas is being pumped out is \( \frac{dV}{dt} = r \). The change in volume would translate to change in the number of moles \( \frac{d(nRT)}{dt} = \frac{dp}{dt} V_0 = -\frac{rRT}{V_0} \). Simplifying, this gives us: \( \frac{dp}{dt} = -\frac{rRT}{V_0^2} \).
03

Solving the Differential Equation

Separate the variables in \( \frac{dp}{dt} = -\frac{rRT}{V_0^2} \) to get \( dp = -\frac{rRT}{V_0^2} dt \). Integrating both sides, we find that \( \int_{p_0}^{p(t)} dp = -\frac{rRT}{V_0^2} \int_{0}^{t} dt \). This results in \( [p(t) - p_0] = -\frac{rRT}{V_0^2}t \), simplifying to \( p(t) = p_0 - \frac{rRT}{V_0^2}t \).
04

Determine Time for Half the Gas to be Removed

Half the gas being pumped out means \( n(t) = \frac{n_0}{2} \). Since \( n_0 \) and \( n(t) \) relate to pressure via the ideal gas law, we have \( p(t) = \frac{p_0}{2} \). Substituting \( \frac{p_0}{2} \) in the expression for \( p(t) \), we have \( \frac{p_0}{2} = p_0 - \frac{rRT}{V_0^2}t_{1/2} \). Solving for \( t_{1/2} \), \( \frac{p_0}{2} = \frac{rRT}{V_0^2}t_{1/2} \). Thus, \( t_{1/2} = \frac{V_0^2}{2rRT}p_0 \).

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Key Concepts

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

Pressure Change
When dealing with gases, the concept of pressure change is crucial for understanding how the state of the gas evolves over time. Pressure is the force exerted by gas particles colliding with the walls of their container and is affected by both the number of particles and the temperature of the system.

In our scenario, as gas is continuously extracted from the container, there is a decrease in the number of gas particles, which leads to a corresponding decrease in pressure. For an ideal gas at constant temperature, we can describe this pressure change using the ideal gas law:
  • Initially, the gas conforms to the relationship \( p_0V_0 = n_0RT \), where \( R \) is the universal gas constant and \( n_0 \) is the number of moles.
  • Over time, as gas is extracted, the volume \( V_0 \) remains the same, but the number of moles decreases, leading to a new pressure \( p(t) \).
This creates a dynamic situation where understanding and predicting how pressure changes with time becomes essential for effective analysis of gas-related processes.
Differential Equation
Differential equations serve as a powerful mathematical tool for describing changes in systems. In our study of gas extraction, a differential equation helps express how pressure changes with respect to time.

Let's break down how the differential equation is used in this context:
  • The extraction rate of the gas, given as \( \frac{dV}{dt} = r \), corresponds to the volume change relation.
  • The corresponding rate of change in pressure is found by differentiating pressure with respect to time, creating the equation \( \frac{dp}{dt} = -\frac{rRT}{V_0^2} \).
By integrating this differential equation, one can determine how pressure changes over time. Integration broadens our ability to solve for \( p(t) \), resulting in a clearer understanding of how varying gas amounts impact pressure. This approach often calls for initial conditions to solve for constants, leveraging the starting pressure \( p_0 \) as reference. The resulting function, \( p(t) = p_0 - \frac{rRT}{V_0^2}t \), illustrates how the pressure diminishes steadily as more gas is pumped out over time.
Rate of Gas Extraction
Understanding the rate of gas extraction is pivotal in quantifying how quickly a gas will exit its container and the subsequent effect on the pressure. The rate offers critical insights into system dynamics.

In this exercise, the extraction rate is noted by the constant \( \frac{dV}{dt} = r \). This value represents the fixed rate at which the gas's volume is decreasing. The rate directly influences how quickly the pressure inside the vessel falls. Key points include:
  • A substantial extraction rate means rapid pressure drop, while a slow rate indicates a more gradual decline.
  • The relationship \( p(t) = p_0 - \frac{rRT}{V_0^2}t \) ties the rate to time-based pressure changes.
To find when half the gas leaves, you solve \( p(t) = \frac{p_0}{2} \), yielding the time \( t_{1/2} \). This derivation from the initial rate showcases how real-world applications check a system's behavior over time, ensuring both accurate predictions and efficient design of processes involving gas extraction.

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Most popular questions from this chapter

Find the number of molecules in \(1 \mathrm{~cm}^{3}\) of an ideal gas at \(0^{\circ} \mathrm{C}\) and at a pressure of \(10^{-5} \mathrm{~mm}\) of mercury.

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