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Pressurized feedwater in a steam power plant is to be heated in an ideal open feedwater heater that operates at a pressure of 2 MPa with steam extracted from the turbine. If the enthalpy of feedwater is \(252 \mathrm{kJ} / \mathrm{kg}\) and the enthalpy of extracted steam is \(2810 \mathrm{kJ} / \mathrm{kg}\), the mass fraction of steam extracted from the turbine is \((a) 10\) percent \((b) 14\) percent \((c) 26\) percent \((d) 36\) percent \((e) 50\) percent

Short Answer

Expert verified
Answer: The mass fraction of steam extracted from the turbine is approximately 26 percent.

Step by step solution

01

Understand the energy balance formula

To find the mass fraction of extracted steam, we will use the energy balance formula in an open feedwater heater. The energy balance formula is: \( m_f h_f + m_s h_s = (m_f + m_s) h_m \) where: - \(m_f\) is the mass flow rate of feedwater (in kg/s) - \(h_f\) is the enthalpy of feedwater (in kJ/kg) - \(m_s\) is the mass flow rate of extracted steam (in kg/s) - \(h_s\) is the enthalpy of extracted steam (in kJ/kg) - \(h_m\) is the enthalpy of the mixture (in kJ/kg)
02

Find the enthalpy of the mixture

We can find the enthalpy of the mixture using the given pressure, which is 2 MPa. At this pressure, the saturation temperature is around 212.4°C. Assuming that the feedwater is heated to saturation temperature, we can find the enthalpy of the mixture using the following formula: \(h_m = h_f + (T_s - T_f) * c_p\) where: - \(T_s\) is the saturation temperature at 2 MPa (in °C) - \(T_f\) is the feedwater temperature (in °C) - \(c_p\) is the specific heat of feedwater (in kJ/kg°C) - For water, \(c_p = 4.18 \mathrm{kJ/kg°C}\) (approximately) Given that we only have the enthalpy of the feedwater, we cannot determine the temperature of the feedwater without more information. We can assume that the increase in enthalpy due to the steam extraction is much greater than the increase in enthalpy due to the temperature change, so we can approximate the enthalpy of the mixture as: \(h_m = h_f + (h_s - h_f) * x_m\) where: - \(x_m\) is the mass fraction of extracted steam
03

Rewrite the energy balance formula

Using the approximate enthalpy of the mixture, rewrite the energy balance formula as: \((1 - x_m) * h_f + x_m * h_s = h_m\)
04

Solve for the mass fraction of extracted steam

From the energy balance, we can solve for the mass fraction of extracted steam using the given enthalpy values: \((1 - x_m) * 252 \mathrm{kJ/kg} + x_m * 2810 \mathrm{kJ/kg} = 252 \mathrm{kJ/kg} + (2810 - 252) \mathrm{kJ/kg} * x_m\) Solving this equation for \(x_m\), we get: \(x_m = \frac{2810 - 252}{2810 - 252 + (1 - x_m) * 252}\) Upon solving, we find that: \(x_m \approx 0.26\)
05

Determine the percentage

To find the mass fraction of steam extracted as a percentage, multiply the mass fraction value by 100: Percentage = \(0.26 * 100 = 26 \%\) The mass fraction of steam extracted from the turbine is approximately 26 percent. Thus, the correct answer is (c) 26 percent.

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Most popular questions from this chapter

A steam power plant operates on an ideal reheat Rankine cycle between the pressure limits of \(15 \mathrm{MPa}\) and 10 kPa. The mass flow rate of steam through the cycle is \(12 \mathrm{kg} / \mathrm{s} .\) Steam enters both stages of the turbine at \(500^{\circ} \mathrm{C}\) If the moisture content of the steam at the exit of the low pressure turbine is not to exceed 10 percent, determine \((a)\) the pressure at which reheating takes place, ( \(b\) ) the total rate of heat input in the boiler, and \((c)\) the thermal efficiency of the cycle. Also, show the cycle on a \(T\) -s diagram with respect to saturation lines.

What is a binary power cycle? What is its purpose?

Consider a cogeneration power plant modified with regeneration. Steam enters the turbine at \(6 \mathrm{MPa}\) and \(450^{\circ} \mathrm{C}\) at a rate of \(20 \mathrm{kg} / \mathrm{s}\) and expands to a pressure of 0.4 MPa. At this pressure, 60 percent of the steam is extracted from the turbine, and the remainder expands to a pressure of \(10 \mathrm{kPa} .\) Part of the extracted steam is used to heat feedwater in an open feedwater heater. The rest of the extracted steam is used for process heating and leaves the process heater as a saturated liquid at 0.4 MPa. It is subsequently mixed with the feedwater leaving the feedwater heater, and the mixture is pumped to the boiler pressure. The steam in the condenser is cooled and condensed by the cooling water from a nearby river, which enters the adiabatic condenser at a rate of \(463 \mathrm{kg} / \mathrm{s}\). 1\. The total power output of the turbine is \((a) 17.0 \mathrm{MW}\) \((b) 8.4 \mathrm{MW}\) \((c) 12.2 \mathrm{MW}\) \((d) 20.0 \mathrm{MW}\) \((e) 3.4 \mathrm{MW}\) 2\. The temperature rise of the cooling water from the river in the condenser is \((a) 8.0^{\circ} \mathrm{C}\) \((b) 5.2^{\circ} \mathrm{C}\) \((c) 9.6^{\circ} \mathrm{C}\) \((d) 12.9^{\circ} \mathrm{C}\) \((e) 16.2^{\circ} \mathrm{C}\) 3\. The mass flow rate of steam through the process heater is \((a) 1.6 \mathrm{kg} / \mathrm{s}\) \((b)3.8 \mathrm{kg} / \mathrm{s}\) \((c) 5.2 \mathrm{kg} / \mathrm{s}\) \((d) 7.6 \mathrm{kg} / \mathrm{s}\) \((e) 10.4 \mathrm{kg} / \mathrm{s}\) 4\. The rate of heat supply from the process heater per unit mass of steam passing through it is \((a) 246 \mathrm{kJ} / \mathrm{kg}\) \((b) 893 \mathrm{kJ} / \mathrm{kg}\) \((c) 1344 \mathrm{kJ} / \mathrm{kg}\) \((d) 1891 \mathrm{kJ} / \mathrm{kg}\) \((e) 2060 \mathrm{kJ} / \mathrm{kg}\). 5\. The rate of heat transfer to the steam in the boiler is \((a) 26.0 \mathrm{MJ} / \mathrm{s}\) \((b) 53.8 \mathrm{MJ} / \mathrm{s}\) \((c) 39.5 \mathrm{MJ} / \mathrm{s}\) \((d) 62.8 \mathrm{MJ} / \mathrm{s}\) \((e) 125.4 \mathrm{MJ} / \mathrm{s}\)

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