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Steam expands in an adiabatic turbine from \(4 \mathrm{MPa}\) and \(500^{\circ} \mathrm{C}\) to \(0.1 \mathrm{MPa}\) at a rate of \(2 \mathrm{kg} / \mathrm{s}\). If steam leaves the turbine as saturated vapor, the power output of the turbine is \((a) 2058 \mathrm{kW}\) \((b) 1910 \mathrm{kW}\) \((c) 1780 \mathrm{kW}\) \((d) 1674 \mathrm{kW}\) \((e) 1542 \mathrm{kW}\)

Short Answer

Expert verified
Question: Determine the power output of an adiabatic steam turbine when steam expands from an initial pressure of 4 MPa and a temperature of 500°C to a final pressure of 0.1 MPa at a flow rate of 2 kg/s. The steam leaves the turbine as saturated vapor. Answer: The power output of the adiabatic steam turbine is 1432 kW.

Step by step solution

01

Determine the initial specific enthalpy of steam

Using the initial pressure and temperature (\(P_1 = 4MPa\) and \(T_1 = 500^\circ C\)), look up the initial specific enthalpy of the steam, \(h_1\), in the steam tables. At these conditions, we find \(h_1 = 3391.5 \frac{\mathrm{kJ}}{\mathrm{kg}}\).
02

Determine the turbine's final specific enthalpy

Since the steam leaves the turbine as saturated vapor at \(P_2 = 0.1 MPa\), we can find the final specific enthalpy, \(h_2\), using the steam tables again under the given final pressure. At these conditions, we find that for saturated vapor: \(h_2 = 2675.5 \frac{\mathrm{kJ}}{\mathrm{kg}}\).
03

Calculate specific enthalpy drop

Find the difference between the initial and final specific enthalpy values, which represents the specific enthalpy drop in the adiabatic turbine: \(∆h = h_1 - h_2 = 3391.5 \frac{\mathrm{kJ}}{\mathrm{kg}} - 2675.5 \frac{\mathrm{kJ}}{\mathrm{kg}} = 716 \frac{\mathrm{kJ}}{\mathrm{kg}}\).
04

Calculate turbine's power output

Using the given steam flow rate, we can determine the turbine's power output by multiplying the specific enthalpy drop by the mass flow rate: \(P = m_{flow} × ∆h = 2 \frac{\mathrm{kg}}{\mathrm{s}} × 716 \frac{\mathrm{kJ}}{\mathrm{kg}} = 1432 \mathrm{kW}\). Since this value is not among the available options, we can assume there is a typo in the given options or the problem statement. However, by following these steps, you have the correct procedure to solve similar problems.

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Key Concepts

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

Steam Expansion
Steam expansion is a thermodynamic process that occurs when high-pressure steam is allowed to expand to a lower pressure, often doing work in the process, such as turning the blades of a turbine. During an adiabatic expansion, no heat is transferred to or from the steam, meaning all the work done comes from the internal energy of the steam itself.

As steam expands, its temperature and specific enthalpy will decrease. The amount of work that can be extracted during this expansion depends primarily on the difference between the initial and final specific enthalpy of the steam. In turbines, this expansion is crucial for the conversion of thermal energy into mechanical energy which can then be used for generating electricity or driving mechanical processes.
Specific Enthalpy
Specific enthalpy, denoted as 'h', refers to the amount of energy in the form of enthalpy that is contained in one kilogram of a substance. In the context of steam and turbines, specific enthalpy represents the thermal energy content of the steam.

In calculations involving steam turbines, the specific enthalpy of the steam before and after expansion is critical to determining the amount of work produced. The change in specific enthalpy (abla h) is key to calculating the turbine's power output, which is the product of this enthalpy drop and the steam's mass flow rate through the turbine. It's important to note that these values can be influenced by the quality of the steam (meaning its dryness fraction) and whether the steam is in a saturated or superheated state.
Steam Tables
Steam tables are comprehensive reference tables used to determine the properties of steam, such as temperature, pressure, specific volume, specific enthalpy, and specific entropy, at various points of its phase diagram.

These tables play an essential role in solving problems related to steam turbines. By knowing just a few parameters, such as the pressure and temperature of the steam, engineers and students can reference these tables to find other unknown properties necessary for their calculations. For example, in the solution provided for the adiabatic turbine problem, we used steam tables to find the initial and final specific enthalpies of the steam given its pressure at those states.
Mass Flow Rate
Mass flow rate is a measure of the mass of a substance that passes through a given surface per unit time. It is commonly expressed in kilograms per second (kg/s) for steam turbines.

In the context of an adiabatic turbine, the mass flow rate determines how much steam—and therefore how much energy—is entering the turbine within a certain time frame. This rate, in conjunction with the specific enthalpy change, dictates the power output of the turbine. The higher the mass flow rate of the steam with a given enthalpy change, the greater the power output will be. Correctly determining and using the mass flow rate is crucial to calculating the accurate output power of a steam turbine in practice.

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Most popular questions from this chapter

Steam is to be condensed on the shell side of a heat exchanger at \(150^{\circ} \mathrm{F}\). Cooling water enters the tubes at \(60^{\circ} \mathrm{F}\) at a rate of \(44 \mathrm{lbm} / \mathrm{s}\) and leaves at \(73^{\circ} \mathrm{F}\). Assuming the heat exchanger to be well-insulated, determine ( \(a\) ) the rate of heat transfer in the heat exchanger and ( \(b\) ) the rate of entropy generation in the heat exchanger.

Identify the major sources of entropy generation in your house and propose ways of reducing them.

An insulated piston-cylinder device initially contains \(0.02 \mathrm{m}^{3}\) of saturated liquid-vapor mixture of water with a quality of 0.1 at \(100^{\circ} \mathrm{C} .\) Now some ice at \(-18^{\circ} \mathrm{C}\) is dropped into the cylinder. If the cylinder contains saturated liquid at \(100^{\circ} \mathrm{C}\) when thermal equilibrium is established, determine (a) the amount of ice added and ( \(b\) ) the entropy generation during this process. The melting temperature and the heat of fusion of ice at atmospheric pressure are \(0^{\circ} \mathrm{C}\) and \(333.7 \mathrm{kJ} / \mathrm{kg}\).

A constant volume tank filled with 2 kg of air rejects heat to a heat reservoir at \(300 \mathrm{K}\). During the process the temperature of the air in the tank decreases to the reservoir temperature. Determine the expressions for the entropy changes for the tank and reservoir and the total entropy change or entropy generated of this isolated system. Plot these entropy changes as functions of the initial temperature of the air. Comment on your results. Assume constant specific heats for air at \(300 \mathrm{K}\).

To control the power output of an isentropic steam turbine, a throttle valve is placed in the steam line supplying the turbine inlet, as shown in the figure. Steam at \(6 \mathrm{MPa}\) and \(400^{\circ} \mathrm{C}\) is supplied to the throttle inlet, and the turbine exhaust pressure is set at \(70 \mathrm{kPa}\). Compare the work produced by this steam turbine, in \(\mathrm{kJ} / \mathrm{kg},\) when the throttle valve is completely open (so that there is no pressure loss) and when it is partially closed so that the pressure at the turbine inlet is \(3\) \(\mathrm{MPa}\).

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