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A piston-cylinder device initially contains \(0.4 \mathrm{kg}\) of nitrogen gas at \(160 \mathrm{kPa}\) and \(140^{\circ} \mathrm{C}\). The nitrogen is now expanded isothermally to a pressure of 100 kPa. Determine the boundary work done during this process.

Short Answer

Expert verified
Based on the given information, the boundary work done during the isothermal expansion of nitrogen gas inside the piston-cylinder device is approximately 37,460 J.

Step by step solution

01

Find the initial volume

We are given the initial pressure, temperature, and mass of the nitrogen gas. We can find the initial volume using the ideal gas law: \(PV = nRT\) First, we need to convert mass to moles and the temperature to Kelvin. The molar mass of nitrogen is 28.02 g/mol: \(n = \dfrac{mass}{molar \thinspace mass} = \dfrac{0.4 kg}{28.02 \frac{g}{mol}} \cdot \dfrac{1000}{1} = 14.275 \thinspace mol\) Next, we convert the temperature to kelvin: \(T = 140 + 273.15 = 413.15 K\) Now, we can find the initial volume using the ideal gas law: \(V_1 = \dfrac{nRT}{P_1} = \dfrac{(14.275 \thinspace mol)(8.314 \frac{J}{mol \cdot K})(413.15 K)}{160 kPa} = 0.478 \thinspace m^3\)
02

Find the final volume

Since the process is isothermal, we can use the same temperature and the final pressure to find the final volume of the nitrogen gas: \(V_2 = \dfrac{nRT}{P_2} = \dfrac{(14.275 \thinspace mol)(8.314 \frac{J}{mol \cdot K})(413.15 K)}{100 kPa} = 0.765 \thinspace m^3\)
03

Calculate the boundary work

When the gas expands isothermally, the boundary work done can be calculated using the following formula: \(W_{boundary} = nRT \ln{\dfrac{V_2}{V_1}}\) Plugging in the values from steps 1 and 2, we get: \(W_{boundary} = (14.275 \thinspace mol)(8.314 \frac{J}{mol \cdot K})(413.15 K) \ln{\dfrac{0.765 \thinspace m^3}{0.478 \thinspace m^3}}\) \(W_{boundary} \approx 37460 \thinspace J\) So, the boundary work done during this isothermal expansion is approximately \(37,460 J\).

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Most popular questions from this chapter

Long cylindrical steel rods \(\left(\rho=7833 \mathrm{kg} / \mathrm{m}^{3}\) and \right. \(\left.c_{p}=0.465 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\right)\) of \(8-\mathrm{cm}\) diameter are heat-treated by drawing them at a velocity of \(2 \mathrm{m} / \mathrm{min}\) through an oven maintained at \(900^{\circ} \mathrm{C}\). If the rods enter the oven at \(30^{\circ} \mathrm{C}\) and leave at a mean temperature of \(700^{\circ} \mathrm{C},\) determine the rate of heat transfer to the rods in the oven.

Consider a well-insulated horizontal rigid cylinder that is divided into two compartments by a piston that is free to move but does not allow either gas to leak into the other side. Initially, one side of the piston contains \(1 \mathrm{m}^{3}\) of \(\mathrm{N}_{2}\) gas at \(500 \mathrm{kPa}\) and \(120^{\circ} \mathrm{C}\) while the other side contains \(1 \mathrm{m}^{3}\) of He gas at \(500 \mathrm{kPa}\) and \(40^{\circ} \mathrm{C}\). Now thermal equilibrium is established in the cylinder as a result of heat transfer through the piston. Using constant specific heats at room temperature, determine the final equilibrium temperature in the cylinder. What would your answer be if the piston were not free to move?

Hydrogen is contained in a piston-cylinder device at 14.7 psia and \(15 \mathrm{ft}^{3} .\) At this state, a linear spring \((F \propto x)\) with a spring constant of \(15,000 \mathrm{lbf} / \mathrm{ft}\) is touching the piston but exerts no force on it. The cross-sectional area of the piston is \(3 \mathrm{ft}^{2}\). Heat is transferred to the hydrogen, causing it to expand until its volume doubles. Determine ( \(a\) ) the final pressure, ( \(b\) ) the total work done by the hydrogen, and ( \(c\) ) the fraction of this work done against the spring. Also, show the process on a \(P\) -V diagram.

A mass of 3 kg of saturated liquid-vapor mixture of water is contained in a piston-cylinder device at \(160 \mathrm{kPa}\) Initially, \(1 \mathrm{kg}\) of the water is in the liquid phase and the rest is in the vapor phase. Heat is now transferred to the water, and the piston, which is resting on a set of stops, starts moving when the pressure inside reaches 500 kPa. Heat transfer continues until the total volume increases by 20 percent. Determine \((a)\) the initial and final temperatures, \((b)\) the mass of liquid water when the piston first starts moving, and (c) the work done during this process. Also, show the process on a \(P\) -v diagram.

Is the relation \(\Delta u=m c_{\mathrm{v}, \mathrm{avg}} \Delta T\) restricted to constant volume processes only, or can it be used for any kind of process of an ideal gas?

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