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Steam enters a long, horizontal pipe with an inlet diameter of \(D_{1}=16 \mathrm{cm}\) at \(2 \mathrm{MPa}\) and \(300^{\circ} \mathrm{C}\) with a velocity of \(2.5 \mathrm{m} / \mathrm{s}\). Farther downstream, the conditions are \(1.8 \mathrm{MPa}\) and \(250^{\circ} \mathrm{C},\) and the diameter is \(D_{2}=14 \mathrm{cm} .\) Determine (a) the mass flow rate of the steam and ( \(b\) ) the rate of heat transfer.

Short Answer

Expert verified
Answer: The mass flow rate of the steam is 50.84 kg/s, and the rate of heat transfer is approximately -3936.88 kJ/s, where the negative sign indicates heat being lost from the steam to the surroundings.

Step by step solution

01

Calculate properties of steam at the inlet and outlet conditions

First, we must determine the properties of steam at the given inlet and outlet conditions. We will need to look up the values of the specific volume (v), enthalpy (h), and internal energy (u) in the steam tables for the given pressures and temperatures. For the inlet conditions, \(P_1 = 2 \mathrm{MPa}\) and \(T_1 = 300^\circ \mathrm{C}\): - \(v_1= 0.0993 \mathrm{m}^3/\mathrm{kg}\) - \(h_{1}= 3038.2 \mathrm{kJ}/\mathrm{kg}\) - \(u_{1}= 2725.2 \mathrm{kJ}/\mathrm{kg}\) For the outlet conditions, \(P_2 = 1.8 \mathrm{MPa}\) and \(T_2 = 250^\circ \mathrm{C}\): - \(v_2= 0.1118 \mathrm{m}^3/\mathrm{kg}\) - \(h_{2}= 2960.9 \mathrm{kJ}/\mathrm{kg}\) - \(u_{2}= 2659.9 \mathrm{kJ}/\mathrm{kg}\)
02

Determine mass flow rate of the steam

To determine the mass flow rate of the steam in the pipe, we will use the continuity equation. Since the velocity and diameter at the inlet and outlet are given, the equation is: \(\dot{m} = \frac{A_1 V_1}{v_1} = \frac{A_2 V_2}{v_2}\) First, calculate the cross-sectional areas at the inlet and outlet: - \(A_1 = \frac{\pi D_{1}^2}{4} = \frac{\pi (0.16 \mathrm{m})^2}{4} = 0.0201 \mathrm{m}^2\) - \(A_2 = \frac{\pi D_{2}^2}{4} = \frac{\pi (0.14 \mathrm{m})^2}{4} = 0.0154 \mathrm{m}^2\) Now, plug in the values and solve for the mass flow rate: \(\dot{m} = \frac{0.0201 \mathrm{m}^2 \times 2.5 \mathrm{m}/\mathrm{s}}{0.0993 \mathrm{m}^3/\mathrm{kg}} = 50.84 \mathrm{kg} / \mathrm{s}\) The mass flow rate of the steam is \(50.84 \mathrm{kg} / \mathrm{s}\).
03

Determine the rate of heat transfer

The conservation of energy equation for a steady-flow process is given by: \(\dot{Q} = \dot{W} + \dot{m}(h_2 - h_1)\) Since there is no work done in this process, \(\dot{W} = 0\), and we can find the heat transfer rate as follows: \(\dot{Q} = \dot{m}(h_2 - h_1)\) Plug in the values for mass flow rate and enthalpy at the inlet and outlet conditions to calculate the heat transfer rate: \(\dot{Q} = 50.84 \mathrm{kg} / \mathrm{s} (2960.9 \mathrm{kJ}/\mathrm{kg} - 3038.2 \mathrm{kJ}/\mathrm{kg}) = -3936.88 \mathrm{kJ} / \mathrm{s}\) The rate of heat transfer is approximately \(-3936.88 \mathrm{kJ} / \mathrm{s}\), where the negative sign indicates heat is being lost from the steam to the surroundings.

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Most popular questions from this chapter

The condenser of a steam power plant operates at a pressure of 0.95 psia. The condenser consists of 144 horizontal tubes arranged in a \(12 \times 12\) square array. Steam condenses on the outer surfaces of the tubes whose inner and outer diameters are 1 in and 1.2 in, respectively. If steam is to be condensed at a rate of \(6800 \mathrm{lbm} / \mathrm{h}\) and the temperature rise of the cooling water is limited to \(8^{\circ} \mathrm{F}\), determine \((a)\) the rate of heat transfer from the steam to the cooling water and ( \(b\) ) the average velocity of the cooling water through the tubes.

Air at \(4.18 \mathrm{kg} / \mathrm{m}^{3}\) enters a nozzle that has an inletto-exit area ratio of 2: 1 with a velocity of \(120 \mathrm{m} / \mathrm{s}\) and leaves with a velocity of \(380 \mathrm{m} / \mathrm{s}\). Determine the density of air at the exit.

A thin-walled double-pipe counter-flow heat exchanger is used to cool oil \(\left(c_{p}=2.20 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\right)\) from 150 to \(40^{\circ} \mathrm{C}\) at a rate of \(2 \mathrm{kg} / \mathrm{s}\) by water \(\left(c_{p}=4.18 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\right)\) that enters at \(22^{\circ} \mathrm{C}\) at a rate of \(1.5 \mathrm{kg} / \mathrm{s}\). Determine the rate of heat transfer in the heat exchanger and the exit temperature of water.

An insulated \(40-\mathrm{ft}^{3}\) rigid tank contains air at 50 psia and \(120^{\circ} \mathrm{F}\). A valve connected to the tank is now opened, and air is allowed to escape until the pressure inside drops to 25 psia. The air temperature during this process is maintained constant by an electric resistance heater placed in the tank. Determine the electrical work done during this process.

Consider two identical buildings: one in Los Angeles, California, where the atmospheric pressure is \(101 \mathrm{kPa}\) and the other in Denver, Colorado, where the atmospheric pressure is 83 kPa. Both buildings are maintained at \(21^{\circ} \mathrm{C}\), and the infiltration rate for both buildings is 1.2 air changes per hour (ACH). That is, the entire air in the building is replaced completely by the outdoor air 1.2 times per hour on a day when the outdoor temperature at both locations is \(10^{\circ} \mathrm{C}\). Disregarding latent heat, determine the ratio of the heat losses by infiltration at the two cities.

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