In this article we will discuss about:- 1. Principle of MHD Power Generation 2. Advantages and Limitations of MHD Power Generation 3. Voltage and Power Output.

Principle of MHD Power Generation:

The magneto hydrodynamic (MHD) power generation is one of the examples of a new unique method of power genera­tion and provides a way of generating electrical energy directly from a fast moving stream of ionized gases without the need for any moving mechanical parts—no turbines and no rotary generators.

The basic principle of MHD generation is the same as that of a conventional electrical generator i.e., the motion of a conductor through a magnetic field induces an emf in it— called the Faraday’s law of electromagnetic induction. In conventional steam power plants, the heat released by combustion of fuel is transformed into internal energy of steam. The steam turbine, then, converts steam energy into mechanical energy used in driving a generator.

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Thus, the mechanical energy is converted into electrical energy. The repeated conversion of various forms of energy involves losses and, therefore, the overall efficiency of thermal power plants is inherently very low. In MHD technology, electrical energy is directly generated from the hot gases produced by the combustion of fuel without mechanical moving parts.

In an MHD generator, electrically conducting gas at a very high temperature is passed at very high velocity through a strong magnetic field at right angle to the direction of its flow, thereby generating electrical energy. The electrical energy is then collected from stationary electrodes placed on the opposite sides of channel. The current so obtained is direct current which can be converted into an ac by an inverter.

Ionized gas can be produced by heating it to a high temperature. On heating of a gas, the outer electrons escape out from its atoms or molecules. The particles acquire an electric charge and the gases passes into the state of plasma. However, to achieve thermal ionization of products of com­bustion of fossil fuels or inert gases, extremely high temperatures are necessary.

Air becomes highly ionized at tem­perature of 5,000° to 6,000°C. To have a reasonable value of electrical conductivity of gases at temperatures around 2,000 to 3,000 K by reasonable ionization, the gases are seeded with additives of easily ionizing materials (alkali metals) such as cesium or potassium.

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MHD system may be an open cycle system or a closed cycle system. In an open cycle system, the working fluid after doing useful work (generating electrical energy) is discharged to the atmosphere through a stack while in a closed cycle system the working fluid is recycled to the heat source and thus used again and again.

The operation of MHD gen­erators directly on combustion products is an open cycle system using air as working fluid. In closed cycle systems gases used on the working fluid are helium or argon.

The use of a nuclear reactor employing solid fuel ele­ments to supply heat energy for an MHD process needs that the working fluid should have the following properties:

(i) It should be capable of providing heat transfer under reactor working conditions.

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(ii) It should not require excessive compressor work.

(iii) It should not be rendered active within the reactor.

Almost all of the above three requirements are fulfilled by helium.

Advantages and Limitations of MHD Power Generation:

MHD power generation offers several advantages over other conventional methods of power generation.

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Some of these are given be­low:

(i) Since high temperatures are involved, operation ef­ficiency is high. MHD system is normally designed to be a topping power system to a conventional steam power plant. At present, the conversion efficiency of an MHD system is around 50% which can be in­creased to 60% with the improvements in experi­ence and technology.

(ii) No moving part, so more reliable.

(iii) Conceptually such generators are much simpler.

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(iv) As there is no limitation to the size of the duct, so high capacity generators are possible.

(v) The walls can be cooled below temperature of working gas.

(vi) Direct conversion of heat into electrical energy re­sults in elimination of the gas turbine (compared with a gas turbine power plant) and both the boiler and the turbine (compared with a conventional steam power plant) and thus in reduction of energy losses.

(vii) Ability of reaching the full power level instantly.

(viii) The more efficient heat utilisation reduces the amount of heat discharged to environments and thus the cooling water requirements are reduced.

(ix) The MHD process is industrially attractive because of the reduced cooling water requirements and at­mospheric pollution.

(x) MHD power generation process is applicable to all kinds of heat sources such as oil, coal, gas, nuclear, solar and thermonuclear fusion.

(xi) MHD power generation offers the flexibility of op­eration in different modes such as base load, peak load or semi-peak load.

(xii) The capital costs of the MHD plants are estimated to be competitive with those of coal fired steam power plants.

(xiii) The overall costs of the MHD power generation are also estimated to be lower (roughly 20%) than those of conventional power plants. This is because of higher efficiency of MHD power generation.

(xiv) The reduced fuel consumption that is obtained because of higher efficiency or better fuel utilisation, offer additional economic and social benefits and also lead to conservation of energy sources.

Inspite of numerous inherent advantages the MHD sys­tem has not been accepted commercially because of the fol­lowing limitations:

1. The efficiencies attained so far have been relatively low.

2. The power output of MHD generator is proportional to the square of the magnetic field density. The electromagnets need very large power for creating strong magnetic fields. The MHD technology is waiting for development of superconducting materials which will need very little power even at ambient temperatures.

3. The combustor, MHD duct, electrodes, and air preheaters are exposed to very corrosive combustion gases at very high temperatures. So, the life of these equipments has been reduced.

4. The ash (or slag) residue from the burning coal is carried over with the combustion gases and tends to cause erosion of exposed surfaces. However, deposition of the slag on such surfaces may also provide some protection.

5. There is a serious problem of separation of seed material from the fly ash and reconversion of potassium sulphate to potassium carbonate.

6. Special fuel gas and preheating of air are required to provide adequate working fluid temperatures.

7. There are serious problems associated with the fabrication of MHD duct, high temperature and high pressure heat exchangers and reactors.

Development of MHD programmes has been undertaken by different countries during the last two decades. In India also considerable studies have been carried out in this field by a team of scientists under the National Council of Sci­ence and Technology (NCST).

The Department of Science and Technology of Govt., of India has sponsored research and development programmes on coal based MHD power generation. Bhabha Atomic Research Centre in collaboration with Bharat Heavy Electricals Ltd and Institute of High Temperature (USSR) is also executing Research and Devel­opment programmes in this field.

The specifications of a Japanese pilot plant (Tokyo) are given below:

Thermal Input : 24 MW

Electrical Input : 1 MW

Mass Flow of Gas : 2.8 kg/s

Flow Velocity : 900 m/s

Duct Length : 1.2m

Inlet : 8 x 10 cm

Output : 8 x 25 cm

Electrodes : 30 pairs

Inlet Pressure : 4 bar

Magnetic Flux Density : 3.5 T (Wb/m2)

Material for Electrodes : Graphite, Water Cooled Copper

Russia has been the pioneer of this new technology. The world’s first U-02 MHD unit was designed by the Russian scientists and power engineers in 1964.

Under intergovernmental agreement, Indian scientists from BARC and power engineers from BHEL worked on a pilot plant of MHD of 5 MW capacity with close interaction with the scientists of the High Temperature Science Institute of Moscow. The pilot plant was set up at BHEL, Trichy.

BARC has developed special magnet MHD duct and power tap-off system. BHEL was responsible for the development and installation of fuel gas generator, oxygen plant, water treatment plant, high temperature regeneration air heaters and valves, the main combustion chamber, nozzles as well as seed injection and seed recovery system.

The main specifications of the pilot plant are as below:

Thermal Input I Stage : 5 MW

                              II Stage : 15 MW

Gas Temperature : 2,600° C

Flux Density : 3 T (Wb/m2)

Seeding Agent : Potassium Carbonate

Electrodes : Water Cooled Copper

Besides the use of MHD system for commercial electri­cal power generation, it has got other special uses. A major effort was made in USA to use MHD as the conversion system in a nuclear electrical system for space crafts. MHD conver­sion has also been considered for ship propulsion, airborne applications, and hypersonic wind tunnel experiments and for many other defence applications.

Voltage and Power Output of MHD Generator:

Lorenz law describing the effects of a charged particle moving in a constant magnetic field can be stated as:

F = QvB …(7.2)

Where F is the force acting on the charged particle, Q is charge of particle, v is velocity of particle and B is magnetic field.

The force on a charged particle moving in an electric field as well as magnetic field will be given as:

F = Q(E + vB) …(7.3)

Where F, E, v and B are vectors.

The velocity in above equation is vector sum of gas velocity v and particle drift velocity u, so force F may be given as:

F = Q(E + vB + u × B) …(7.4)

= Q(E’ + u × B) …(7.5)

Where E’ = E + vB

Consider Fig. 7.5, the motion of gas is in x direction, magnetic field B is in y direction and force on the particle in z direction. A load resistance RL is connected across the electrodes (plates P1 and P2).

When a current I flows through the load resistance RL, then electric field intensity between the electrodes is given as:

Ez = – V/d …(7.6)

Where d is the distance between the plates.

Total Electric Field E’z =  Ez + Bv

= V/d + Bv = 1/d (Bvd – V)….. (7.7)

The electromagnetic field Ez and B acting on the moving gas develops the same force on the ions as electromagnetic field E’z and B develops on a gas with zero average velocity. Obviously the term Bvd provides the internal emf or open-circuit voltage E0 of the MHD power generator i.e.,

E0 = Bvd …(7.8)

If RG is the internal resistance of the generator, then maximum power output will be obtained when RG = RL.

MHD system is reversible process. If load resistance RL is replaced by emf E greater than E0 by shifting the switch from position 1 to position 2, the directions of flow of current and force experienced on the ions will be reversed and the system will accelerate the gas particles because energy would be supplied to gas.

Thus, the ejected gas would be at a higher velocity than the inlet gas. The reaction force experienced on the magnet would tend to push the MHD engine in the negative x direction and thus the electrical energy would be converted into mechanical energy.