DE1488424C - Method for operating a cross-connected MHD generator or a Hall MHD generator - Google Patents

Description

The invention relates to a method for operating a cross-connected MHD generator or Hall MHD generator, in which the electric field strength has an essential component (E _x ) in the direction of the flow vector of the working medium.

The purpose of the invention is to create a relatively simple and straightforward one to operate MHD generator, which, according to its economic efficiency, can also be used in large systems, such as B. power plants, can be used.

The object of the invention is to provide a method for operating an MHD generator, which compared to the known generators described below mainly by a higher overall efficiency.

Based on the known method cited at the beginning, this object is achieved according to the invention solved that the generator is divided into partial generators in the direction of the flow vector and a part of the current at the output of each partial generator

is tapped, and that the through e _H =

ned characteristic load factor, whose absolute value! ff / 1 ^m near the input of each sub-generator has a maximum and near the output a minimum, by regulating the tapped currents and varying the length of the sub-generators in the direction of the working medium flow for the maximum points to 0.2 <| ε _Η \ < 0.35 and is set to 0.1 < \ e _H \ < 0.25 for the minimum digits.

Using the drawings and the theoretical considerations developed below, the Invention explained in more detail.

In order to get a first approximation of the conditions in MHD generators, one can first of all consider the behavior of generators with a flat working medium flow, with the magnetic Induction normal to which the flow is assumed. This case of plane flow became theoretical already dealt with in detail, e.g. B. von B ü r g e 1 (BB. Mitt. 1962, p. 493), whose nomenclature is in the The following description has essentially been adopted.

The following applies as a first approximation:

Hall parameter β =

Q ₀ B

n " ■ e

σ ₀ scalar electrical conductivity,

n _e density of free electrons,

jB magnetic induction,

ι / flow velocity,

e elementary charge.

The x-direction is by definition (FIG. 1) the direction of the flow velocity w. The induction B points downwards (neg. Z-axis), but is usually used positively. The relationship between the stroke density vector J " (A / m ² ) and the electric field vector E (V / m) is then given by the following pair of equations:

J, - γ ** Ά *

1 + ß ²

\ _- β E _x + (E _x + 1/5)]. (3)

These equations can be graphically represented in pie charts according to Bürge 1, ζ. Ε F i g. 2 for β = 5; F i g. 3 for β = 10. Locations constant! Efficiency are circles; ζ. Β. η = 0.7 ... 0.8 entered as the area of interest. The power density is greatest in the center Z and decreases with the square of the radius to the value 0 on the large circle.

A well-known special case of an MHD generator: the so-called "Faraday generator", as shown in FIG. 4 of the drawing formed and z. B. from British patent specification 987 590 or from French patent specification 1 308 804 can be found. Since there are enough freely selectable dimensions available with this type of generator, there are no difficulties in achieving usable dimensions , even with quantities p, T, σ and f that vary greatly in the direction of flow. In the case of generator designs, in particular according to FIG. 1 of the last-mentioned patent specification or according to FIG. 4 of the present application, it is now significant that each load is connected separately to a pair of electrodes, so that each load can be optimally adapted to the operating conditions. This type of generator therefore requires correspondingly many or too many independent loads and is therefore too complicated and too expensive to be able to be used efficiently, particularly in a larger system, for example in a power plant with 100 individual loads or more. The generator type in particular according to FIG. 2 of British patent specification 987 590 probably has a switched on or off by means of a switch. bare straight-line connection, which only serves to briefly close the two independent loads at the two ends of such a generator in order to facilitate the disconnection of the load currents and thereby make them disappear. The last-mentioned type of generator therefore has a mode of operation that changes over time, as can also be seen from claim 1 of the aforementioned British patent, whereas the subject matter of the invention is essentially an operation that does not change over time.

The literature is also available through the journal Proceedings IEE, No. 10, October 1963 the pp. 1837 to 1854, in particular from F i g. 3 on p. 1840, as well as from Fig. 6 of the drawing of the "Hall generator" as a special case of the to illustrate the state of the art in FIG. 5 of the drawing cross-connected generator known.

The cross-connected generator or the Hall generator generally has only one or a few few, generally less than 10 in parallel Loads on The current of this one load or each of these loads connected in parallel flows from one end of the generator to the other and is therefore subject to the continuity condition of the current (See equations 8 and 11 below), which results in a deterioration in efficiency for such generators results.

The object of the invention now aims to improve the cross-connected generators (FIG. 5) or the Hall generators (FIG. 6), in order to ensure efficient use of these in and of themselves in operation so complicated generators to enable.

The essential advantage achieved with the invention consists in particular in the aforementioned effect

degree deterioration, especially in the case of operation that does not change over time, as a result of the Measures to avoid.

If one uses the circle diagrams in FIG. 1 to examine the generator operating conditions. 2 and 3, the operating points of Faraday generators are obviously on the straight line F, those of Hall generators on the Geiaden H. An additional continuity condition has to be fulfilled for the cross-connected generator, which has not been observed up to now.

Although the continuity condition can also be represented mathematically for the general case can, should be the restriction in the free choice of company sizes imposed by this condition will be made plausible on the basis of two special cases:

Case a

First of all, the cross-connected generator is considered, namely the case that j _x = 0 everywhere. Then from (2) and (3) one obtains:

E _x = -β (E _y + uB), j, = a _o (E _y + uB) = a _o uB (e + l);

(4)

(5)

Let us also assume a square channel a ² - A. The electrodes are connected crosswise; in Fig. Figure 7 shows K such a connection; the others are only indicated by arrows. These connections give equipotential lines, e.g. B. e ,, e ₂ , e ₃ ... perpendicular to this are the field vectors E *. The angle φ results from F i g. 2 and 3 and with (4) and (5) immediately

The length of a sector (with parallel, independent electrodes) in FIG. 7 will

L = α tg φ =

- α ε

The current J enters the channel from the lower electrodes of a sector and goes to the electrodes on the opposite side. From there, the current is passed externally to the lower electrodes of the next sector, where it re-enters the channel.

J = L- aj _y = -

α σ ₀ uB (e + 1)
(* + 1) ß

σ ₀ n _e ■ e

(from 1) and

(6)

Au ρ = m

ρ = density of the gas

and

will

m = mass flow of the gas

J = · e ■ n _e ■

From the continuity condition J ₁ = J ₂ follows

KIo) ₂

So one is no longer free to choose ε as in the Faraday generator. Since n _e now depends exponentially on T , n _e 'falls along the generator much more rapidly than o, ie f ₂ / fi> 1. So f increases inevitably. At the generator input, e must already be 0.65 ... 0.8, since η % is e . e then rises rapidly to 1 (power density 0) and above (motor instead of generator).

Case b

The same applies to the Hall generator. With E _y - 0 gives (2)

β uB].

According to FIG. 1, the Hall generator achieves. 2 and 3 only good efficiencies η for large ß values, since only then does the line H intersect the circles with good η. It is therefore justified for the following basic presentation to neglect 1 blessing ß ^2. With (.1) becomes (9):

= n- e

(10)

ßuB- With the continuity equations

J _x ■ A = J _x

u-A = m

surrendered

(M ± -ι

\ fnej n _e

(H)

(12)

At the entrance, again because of the need to choose a good r _h e _{H, it is} approximately -0.2 ... -0.35. So the first link on the right in (12) has the size 0.65 ... 0.8. ο , as already explained, falls much more slowly than t / _e , and the first link grows. E _H = 0 and then becomes positive; the channel then no longer acts as a generator.

The formulas (7) for case a and (12) for case b show, as a consequence of the mentioned continuity condition, that neither i- nor / _{; /} can be influenced by u or B. An additional injection of seed material could act on n _e, but is unlikely to be economical.

At a certain cross-section of the generator, the load factors f and i- _{H reach a value which corresponds to insufficient efficiency.}

The overall efficiency of the generator is now increased in the manner according to the invention in that t and ε _Η from this cross-section onwards are brought back to usable values by current tapping at this cross-section, ie by lowering the current flowing through the cross-section [s. equations (7) and (12)], or in other words: that the generator is divided into sub-generators in the direction of the flow vector of the working medium, with current being tapped at the output of each sub-generator.

The load factor e _H = - ^ not only gives the ver

15th

conditions in pure Hall generators, but also characterizes the behavior of generators well, where in general the electric field strength has an essential component in the direction of the flow vector of the working medium (E _x ).

The above considerations are also not valid for the general cross-connected generator of the linear type, where the current can be drawn off via existing electrodes of the cross-connection, but also for generators with rotationally symmetrical flow, in which there are no separate electrodes for Hall or cross connection, since the tangential electrical current closes itself within the flow of the working medium (see Fig. 8). The following should also be noted about the course of \ e _H \ at the boundary of two sub-generators: Due to the current tapping, \ ε _Η \ undergoes a strong change along a short distance that is about the order of magnitude of the width of the tapping electrode and is of a minimum value, which lies in the vicinity of the output of the upstream sub-generator, is raised to a maximum value in the vicinity of the input of the adjoining, downstream sub-generator. e _H can be determined at these extreme points without any particular difficulty.

Claims (1)

Claim: Method for operating a cross-connected MHD generator or a Hall MHD generator, in which the electric field strength has a substantial component (E _x ) in the direction of the flow vector of the working medium, characterized in that the generator is divided into sub-generators in the direction of the flow vector a part of the current is tapped at the output of each sub-generator E.
becomes, and that the one defined by ε _Η = jt> characteristic load factor whose absolute value | f _H | has a maximum near the input of each sub-generator and a minimum near the output, by regulating the tapped currents and varying the length of the sub-generators in the direction of the working medium flow for the maximum points to 0.2 <| * · _Η | <0.35 and for the minimum digits to 0.1 <| f _h | <0.25 is set. 1 sheet of drawings