Appendix 1 MHD shock wave suppression concept

science/mhd

Appendix 1: MHD

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1 - Generalities on the concept of shock wave cancellation

This was introduced in the beginning of the seventies. Then the US government understood that MHD could play an important role in future military projects. At the same time the US scientists understood the MHD had something to do with hypersonic flight. They decided to desinform people. Officially, in USA, MHD was abandoned. Civil MHD got starved. Big industrial projects were abandoned. But, at the same time, an intensive effort began, in full secrecy, about military MHD. This was discovered very recently (2001). The reader is free to believe or not to believe this. We were told about what happened in US between 1970 and the present days by top level American scientists involved in secret black programs, concentrated in area 51. The only argument about this is based on scientific grounds. Even now, people ignore many very important features about MHD applied to supersonic gas flows, which made possible a fantastic and fundamental breakthrough in USA in the middle of the seventies. Thirty years after American mastered the world with advanced technologies in many (military) fields, including long duration hypersonic flight, up to Mach 12.

I don't know who will read this annex, whose reading requires advanced knowledge in supersonic fluid mechanics, characteristic theory and MHD. A very good book was published in 1967, entitled "Engineering Magnetohydrodynamics"; Sutton and Sherman, Mac Graw Hill Books Company.

Let us present some basic concepts.

In a supersonic flow we may consider "Mach Lines" :

Mach lines

Mach lines (or Mach surfaces) in a supersonic flow

The angle of such Mach line depends on the local value of the velocity.

rising velocity

Impact of the velocity rising of the Mach angle

If we consider a supersonic flow, Mach lines, "characteristic lines" are real. They map the flow. Next, a 2d supersonic test nozzle (supersonic wind tunnel).

supersonic nozzle

In the convergent section the fluid is in subsonic condition. From a mathematical point of view the characteristic lines, (the Mach surfaces) are imaginary. The velocity of the sound is reached at the throat of the nozzle. Then the Mach surfaces become real. We can figure it :

supersonic nozzle2

Evolution of Mach surfaces, or Mach lines in a supersonic nozzle.

In the nozzle the velocity grows continuously. At the same time the Mach angle decreases (it is equal to 90° at the throat section). It corresponds to the "natural variation" of the Mach surfaces system, due to the expansion of a supersonic flow.

Now, consider a 2d supersonic flow around a flat wing. We may compute the theoretical Mach lines system, through characteristic theory:

characteristic flat wing

Theoretical characteristic lines around a flat wing imbedded in a supersonic gas flow.

This is not physical. That's "pure mathematics" (a solution of a "characteristic system). It shows how the characteristic surface collide, accumulate in some place. They are elementary pressure variation characteristic surfaces. In the middle of the flow we see a classical expansion fan, where the pressure gets lower and where the gas is accelerated. But in another regions we see how the Mach surfaces accumulate and tend to give attached shock waves. The next figure corresponds to really physical solution, with subsequent attached shock waves :

flat shock waves

Physical conditions with attached oblique plane shock waves.

Next : these flat attached shock waves.

Next, these flat waves, plus flow lines.

If the leading edge is sharp the front waves are attached. See detail :

attached front shock detail

Attached front shock wave at the vicinity of the leading edge of a flat wing

If the leading edge is blunt the situation is somewhat different. The shock looks like a bow.

blunt wing

Shock wave at a blunt leading edge.

From a classical point of view these shock waves cannot be avoided. They correspond to pressure and temperature jumps. When the Mach number becomes higher than 3 material cannot stand the heat flux and gets vaporized. In "scramjets" one cools the leading edge with liquid hydrogen and oxygen, which makes possible to achieve short duration Mach 5-6 flight. But hypersonic flight (Mach 12) is considered as impossible, on technological grounds. In 1947 the ufo phenomenon arose a strange question : is it possible to achieve such high Mach number flights ? In Roswell Americans got the crashed machine, which proved immediately two things :

  • Ufos were definitively real

  • They came from other planetary systems.

It was decided to keep a full secrecy about that. An intense and active policy of disinformation was built up in USA, which is still in action. NASA, for example, in its official website explains that ufos are nothing but an illusion, almost 50 years after. It took time to Americans to understand that MHD was the key, the master word of the hypersonic (and silent) flight. The silent flight of ufos showed that shock waves (and turbulence) were avoided. To illustrate that we shall refer to the author's personal works (extending during the sixties and seventies). This research was done with quite modest lab's equipment, compared to the huge US effort, hidden in underground area 51 plants. But this will be enough to show the basic ideas. On the next figure a "Faraday MHD linear converter" with its MHD channel and its two coils.

Faraday converter

Faraday MHD converter

If we remove the two coils we get that :

Faraday channel

Faraday channel (the coils have been removed)

Here the converter acts as a MHD generator. The supersonic flow enters the channel at velocity V, which goes with an induced electric field E x B . This last produces an electric current in the gas, which loops through external loads, shown. A part of the kinetic energy of the gas can be converted into electricity. This goes with the slowing down of the gas. The system of Velocity, Electric Field and subsequent Lorentz force is shown next :

Faraday channel forces

Electric field and Lorentz force field in a MHD generator.

The Lorentz force obeys the "three fingers' rule" :

three fingers law

This first idea is very important. In effect we see that a MHD accelerator slows down a supersonic fluid. If conveniently managed we can imagine that the fluid parameters can be modified in a "soft way",

without shock wave birth.

That is the key idea of the hypersonic flight concept, as will be shown further. Next we show the characteristic pattern of Mach lines in a MHD generator. The Mach angle changes continuously and no shock occurs.

characteristic slowing down

Shockless modification of the Mach lines system, due to Lorentz force action

This is a very simple idea, but it was considered as top secret during a very long time over all the world. On another hand, a MHD converter can be used as an accelerator. To do that we just inject electric power in order to inverse the electric current and get accelerating Lorentz forces. Then we can modify the local value of the Mach angle. In my lab, in 1967 we got very impressive accelerations along very small length.

increasing velocity

The gas enters the channel on the left and Lorentz forces accelerates it.

Let us show that this was not a dream. Next, my MHD lab in the sixties at the Institute of Fluid Mechanics of Marseille, France. .

TC8

My MHD lab in the sixties. Front : electrodes. Left, an old Tektronix vacuum lamps oscilloscope. Below : the Faraday converter with

hung coils. Besides, an "ignitron" used to commute the 50,000 amperes electric current produced by a capacitor bank.

It was a "short duration wind tunnel" based on a "shock tube". A shock driven argon flow (200 microseconds) was pushed in a 6 meters long constant area wind tunnel. The gas was moved and compressed (pressure after compression : one bar). The gas was heated up to 10,000°K, which provided a very good electrical conductivity (3000 mhos/m). The velocity of the gas, at the entrance of the MHD channel was 2,750 m/s. This last was 10 cm long. When carrying up acceleration experiments the exhaust velocity reached 8,000 m/s, which demonstrated the extraordinary efficiency of Lorentz forces accelerating power with high magnetic field strength (2 teslas) and high electrical current densities. Next, the classical MHD efficiency :

MHD efficiency

MHD efficiency. J is the electric current density, B is the magnetic field, L is a characteristic length, below : the mass density and v the velocity.

At the beginning of the eighties a French engineer, Bertrand Lebrun, started a PhD with me. I defined the basic idea of the shockless supersonic flight. This was a civilian research but we know that similar research was carried in secrecy in the famous Lawrence Livermore Laboratory, California, at the same time. We have already presented the general pattern of Mach lines, associated to the theoretical supersonic flow around some flat wing. We have seen that we could change the local value of the Mach angle by a subsequent choice of a convenient Lorentz force Field. For example we can accelerate the flow around the leading edge, using a transverse magnetic field and two wall electrodes, as following :

leading edge electrodes

Accelerating electrodes, at the vicinity of the leading edge

Next, the subsequent Lorentz force field :

leading edge forces

Lorentz force field

With such device it was possible to cancel the front shock wave at the vicinity of a sharp leading edge which showed that a shock system could be avoided. This changed drastically the problem of the hypersonic flight. Now the goal was to cancel and shock around a flat wing, which implied to keep the Mach lines parallel :

flat wing the goal

Lebrun PhD : the goal

Three couples of wall electrodes were arranged on the flat wing model :

electrodes on flat wing

Lebrun PhD thesis (1987)

Up : the idealized characteristic lines pattern (Mach lines of Mach surfaces). If a convenient Lorentz force field could be applied around the model it was expected that a characteristic line focusing phenomenon could be avoided. This was shown through computer calculations and presented at several international MHD meetings (Tsukuba, Japan, Beijing, China, see bibliography and mentioned papers). The general pattern of Mach lines becomes the following :

Lebrun phd

Lebrun PhD thesis. Characteristic lines.

This work was done in a civilian laboratory but we know that at the same time Americans did the same stuff in high level of secrecy. In France the officials were deadly scared that such results could evidence the extraterrestrial nature of ufos and they became mad at it. All the civilian research was ended. The military tried to continue this research in their secret labs, for their own, but they failed, due to their lack of knowledge. During this time the US projects experienced a very strong acceleration. Parallel research was intensively carried, about torpedos and submarine propulsion. To avoid to confuse the mind of the reader we will talk about that further.

Bibliography

:

(1)

J.P. Petit

: "Is supersonic flight possible ?" Eighth Inter. Conf. on MHD Electr. Power Generation. Moscow 1983.

(2)

J.P. Petit & B. Lebrun

: "Shock wave cancellation in a gas by Lorentz force action". Ninth Inter. Conf. On MHD Electr. Power Generation. Tsukuba, Japan, 1986

(3)

B. Lebrun & J.P. Petit

: "Shock wave annihilation by MHD action in supersonic flows. Quasi-one dimensional steady analysis and thermal blockage". European Journal of Mechanics; B/Fluids, 8 , n°2, pp.163-178, 1989

(4)

B. Lebrun & J.P. Petit

: "Shock wave annihilation by MHD action in supersonic flows. Two-dimensional steady non-isentropic analysis. Anti-shock criterion, and shock tube simulations for isentropic flows". European Journal of Mechanics, B/Fluids, 8 , pp.307-326, 1989

(5)

B. Lebrun

: "Approche théorique de la suppression des ondes de choc se formant autour d'un obstacle effilé placé dans un écoulement d'argon ionisé. Thèse d'Energétique n° 233. Université de Poitiers, France, 1990.

(6)

B. Lebrun & J.P. Petit

: "Theoretical analysis of shock wave annihilation by Lorentz force field". International MHD symposium, Beijing 1990.

Annex 1 (MHD), next page

![shock waves](/legacy/Disclosure/Annex_MHD1/Annex_MHD1_figures/shock waves.jpg)

![oblique shock waves](/legacy/Disclosure/Annex_MHD1/Annex_MHD1_figures/oblic shock waves.jpg)