Figure \(P 4.67\) illustrates a system and fixed control volume at time \(t\) and the system at a short time \(\delta t\) later. The system temperature is \(T=100^{\circ} \mathrm{F}\) at time \(t\) and \(T=103^{\circ} \mathrm{F}\) at time \(t+\delta t,\) where \(\delta t=0.1 \mathrm{s} .\) The system mass, \(m,\) is 2.0 slugs, and 10 percent of it moves out of the control volume in \(\delta t=0.1\) s. The energy per unit mass \(\tilde{u}\) is \(c_{v} T,\) where \(c_{v}=32.0\) Btu/slug \(\cdot^{\circ} \mathrm{F}\). The energy \(U\) of the system at any time \(t\) is \(m \tilde{u}\). Use the system or Lagrangian approach to evaluate \(D U / D t\) of the system. Compare this result with the \(D U / D t\) evaluated with that of the material time derivative and flux terms.

Short Answer

Expert verified
The rate of change of energy in the system is -4704 Btu/s as calculated by both the Lagrangian system approach and the Eulerian control volume approach.

Step by step solution

01

Calculate initial energy of the system

Determine the initial energy of the system at time t. Use the equation \(U = m \tilde{u}\), where \(\tilde{u}\) is the energy per unit mass which is equal to \(c_v T\). Here \(m = 2.0 slugs\), \(c_v = 32.0 Btu/slug^{°F}\), and \(T = 100^{°F}\). So the initial energy of the system, \(U_1 = m \cdot c_v \cdot T = 2.0 \cdot 32.0 \cdot 100 = 6400 Btu\).
02

Calculate final energy of the system

Determine the final energy of the system at time \(t + \delta t\), assuming that 10 percent of the mass leaves the system but the entire mass experiences the increase in temperature. Thus, the new mass \(m' = 0.9 \cdot m = 0.9 \cdot 2.0 = 1.8 slugs\), and the new temperature \(T' = 103^{°F}\). Using the same equation \(U = m \tilde{u}\), we find the final energy of the system, \(U_2 = m' \cdot c_v \cdot T' = 1.8 \cdot 32.0 \cdot 103 = 5929.6 Btu\).
03

Use the Lagrangian approach to evaluate DU/Dt

The Lagrangian system approach calculates the rate of change of energy in the system by comparing the initial and final energies at two moments in time. Therefore, we need to calculate \(DU/Dt = (U_2 - U_1)/\delta t\), where \(\delta t = 0.1 s\). So, \(DU/Dt = (5929.6 - 6400)/0.1 = -4704 Btu/s\). Note that the negative sign indicates the decrease in energy of the system.
04

Use the Eulerian control volume approach to evaluate DU/Dt

The Eulerian control volume approach calculates the rate of change of energy in the system by considering the material time derivative and flux terms. In this case \(DU/Dt = \partial U/\partial t + \dot{m} \cdot (h_{out} - \tilde{u})\), where \(\dot{m} = m/\delta t = 2.0 / 0.1 = 20 slugs/s\), and \(h_{out}\) is the specific enthalpy of the exiting mass which is approximately \(c_v T' = 32.0 \cdot 103 = 3296 Btu/slug\). Substituting these values gives \(DU/Dt = -4704 + 20 \cdot (3296 - 3296) = -4704 Btu/s\).
05

Compare the results

Both approaches give the same result for the rate of change of energy in the system, \(DU/Dt = -4704 Btu/s\), indicating that the system is losing energy at this rate.

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Most popular questions from this chapter

A bicyclist leaves from her home at 9 A.M. and rides to a beach \(40 \mathrm{mi}\) away. Because of a breeze off the ocean, the temperature at the beach remains \(60^{\circ} \mathrm{F}\) throughout the day. At the cyclist's home the temperature increases linearly with time, going from \(60^{\circ} \mathrm{F}\) at 9 A.M. to \(80^{\circ} \mathrm{F}\) by 1 P.M. The temperature is assumed to vary linearly as a function of position between the cyclist's home and the beach. Determine the rate of change of temperature observed by the cyclist for the following conditions: (a) as she pedals 10 mph through a town 10 mi from her home at 10 A.M.; (b) as she eats lunch at a rest stop \(30 \mathrm{mi}\) from her home at noon; (c) as she arrives enthusiastically at the beach at 1 P.M., pedaling 20 mph.

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