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as in a uniform magnetic field and the other is the oscillatory part with a comparable

order of

magnitude.

The pressure drop takes place proportional

to the power output as the velocity of

the main flow exceeds that of the progressing

magnetic field. The pressure drop due to the

boundary

layer loss is small, on the order of R- ‘I2 . These results should be useful as

fundamental

knowledge

when we consider

a liquid metal induction

generator

and MHD

metallurgy problems and also when we carry out numerical calculations

for more general cases

of Reynolds number and magnetic Reynolds number.

2. Flow configuration

Fig. 1 shows the flow of an incompressible

conducting

fluid between two parallel walls in the

presence of a progressing alternating

transverse magnetic field. The rectangular

wave profile in

the figure denotes the stator that produces

a progressing

alternating

magnetic

field. Two

parallel walls are made of insulator of sufficient thinness and located close to the stator. If we

supp

order of

magnitude.

The pressure drop takes place proportional

to the power output as the velocity of

the main flow exceeds that of the progressing

magnetic field. The pressure drop due to the

boundary

layer loss is small, on the order of R- ‘I2 . These results should be useful as

fundamental

knowledge

when we consider

a liquid metal induction

generator

and MHD

metallurgy problems and also when we carry out numerical calculations

for more general cases

of Reynolds number and magnetic Reynolds number.

2. Flow configuration

Fig. 1 shows the flow of an incompressible

conducting

fluid between two parallel walls in the

presence of a progressing alternating

transverse magnetic field. The rectangular

wave profile in

the figure denotes the stator that produces

a progressing

alternating

magnetic

field. Two

parallel walls are made of insulator of sufficient thinness and located close to the stator. If we

supp

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