Original Article

, Volume: 6( 1)

# The Processes of Energy/Momentum Exchange for Rotating Plasma Flows in Crossed External Fields

**Karimov AR ^{1*} and Murad PA^{2}**

^{1}Russia Department of Electrophysical Facilities, National Research Nuclear University MEPhI, Kashirskoye Shosse 31, Moscow, Russia

^{2}Morningstar Applied Physics, LLC Vienna, VA 22182, USA

- *Correspondence:
- Karimov AR , Russia Department of Electrophysical Facilities, National Research Nuclear university MEPhI, Kashirskoye Shosse 31, Moscow, 115409, Russia,
**Tel:**+74991357760;**E-mail:**[email protected]

**Received:** December 07, 2016; **Accepted:** February 16, 2017; **Published:** February 23, 2017

**Citation:** Karimov AR, Murad PA. The Processes of Energy/Momentum Exchange for Rotating Plasma Flows in Crossed External Fields. J Space Explor. 2017;6(1):113.

### Abstract

The processes of energy/momentum exchange in rotating plasma flows placed into crossed magnetic and electric fields is an issue of importance. Such flows are capable of transforming the energy from different degrees of freedom into another. The resulting energy and momentum from one degree can be altered owing to the interaction of the coupled nonlinear radial, axial and azimuthal electron-ion oscillations. These processes may lead to the acceleration of flow in the axial direction with these stable effects. This technology can be instrumental for creating efficient thrusters employing pulse transformations manipulated by the electric and magnetic fields. This would be suitable for space propulsion and other environmental effects.

### Keywords

*Rotating plasma flow; Energy/momentum exchange; Intermodal exchange; Crossed magnetic field*

### Introduction

**The problem to be analyzed**

The behavior of rotating flows in crossed physical fields is of interest for different technical applications and natural phenomena. For example, in the Hall thrusters the orthogonal electric and magnetic fields are used to produce thrust by altering the behavior of plasma [1-8]. As a result, the electrons can experience rotation or the Poynting vector in the azimuthal direction and shift ions to move only in the axial direction. Thus, a radial magnetic field confines rotating electrons which compensate the space charge of the flow, while an axial electric field alters by accelerating the motion of the electrons. The similar mechanisms may be related to the acceleration of the high-energy jets near black holes and pulsars where one should take into account the gravitational fields [9-11]. These examples show that any combination of electric, magnetic, non-inertial and gravitational fields may propel unusual processes of energy/momentum transfer. This allows us to speak about redistribution of energy/momentum between the macroscopic degrees of freedom of the macroscopic flows.

As an object of such a kind, the present paper takes a cylindrical plasma flow in an external magnetic field. Such rotating plasma flow is one of simple physical patterns, however, manifesting different nonlinear wave-like properties owing to the electron and ion fluids may be treated as a set of coupled nonlinear radial, axial and azimuthal oscillators of different kinds that define the variety of wave forms. On the other hand, there are a numerous technical applications including plasma Hall thrusters where such flows have been applied.

There are two principally different physical situations for the development of such nonlinear wave-like phenomena. First, one can expect the emergence of wave-type behavior when the initial state coincides with one of the equilibrium states. In this case, well-known weakly nonlinear waves may be observed [12-14]. However, for initial states not close to equilibria, such an approach is inadequate and one can try to investigate wave-like behavior near some time-dependent state [15-21]. Such states, in the form of highly nonlinear plasma oscillations and patterns, are little understood but have indeed were shown to exist [20-25]. Following these works, we will consider some features of energy/momentum transfer for such nonequilibrium plasma flows and discuss the applications of these effects for a accelerating propulsion facility or natural phenomena.

### Asymmetric plasma flow in the crossed magnetic fields

The proposed scheme of this plasma flow is presented in **Figure. 1**. In this experiment, one can make such a configuration of magnetic fields with the help of a solenoid ( *B _{z0}* ) and permanent magnets (

*B*). The change of axial magnetic flux can induce an azimuthal electric field that rotates electrons and ions in different directions as seen in

_{r0}**Figure. 1**. Such a type of azimuthal acceleration is known as an induction acceleration widely used in accelerator technology. The azimuthal electron and ion flows interact with the radial component (

*B*) via the Lorentz force, this leads to the axial acceleration of electrons and ions in the axial direction. Owing to this process, the transformation of azimuthal momentum transfers into axial momentum. Despite the difference in the electron

_{r0}*m*and ion

_{e}*m*, masses the electron and ion fluids can move together due to the action of the inherent electric fields of the plasma.

_{i}To understand the behavior of the flow depicted in **Figure. 1**. we will study the following model with an azimuthally symmetric plasma where but will include the azimuthal components in the electric and magnetic fields. We will propose there is an additional external spatially homogeneous magnetic field which depends only on time.

where* B _{r0}* (t) and

*B*(t) are some known functions. Such an external magnetic field induces an electric field which can possibly rotate electrons and ions in different directions if the model is successful.

_{z0}With the linearity of the Maxwell equations, we can present the total electric and magnetic fields of the system. Let us assume we have mean values with a perturbation such as:

and

,

Where the perturbed electric and magnetic fields are defined by the dynamic processes in itself plasma medium described by the standard cold-fluid model in the dimensionless form.

, (1)

, (2)

Here and , where the label *s* = *e* relates to the electron fluid and the label *s* = *i *- to the ion fluid. The perturbed fields are defined by

The perturbed fields are defined by

, (3)

, (4)

, (5)

(6)

Where is the electron density, is the ion density, is the electron fluid velocity, is the ion fluid velocity?

To write these equations in terms of dimensionless variables, let the initial electron density , the initial radius of plasma cylinder *R _{0}* , the inverse electron frequency , where

*e*is the electric charge, as the natural scale of all densities, coordinates and time.

All velocities are normalized by the , the electric field normalized by the and the magnetic field is normalized by the , where c is the speed of light.

From equation of induction (6) written for external magnetic field in integral form

this follows that the external electric field has only an azimuthal component determined by

(7)

This relation suggests to seek the possible solution of the governing set in the form

(8)

Also, supposing that the intrinsic electric field of the system is similar to the velocity field (8), we can write

(9)

And set

. (10)

In this case, from (6) follows that

, (11)

i.e. for the initial conditions . Only the component may be distinct from zero inside the plasma cylinder and the one is the function of time. It means that = 0. Moreover, substituting (9) and (10) into Eq. (5) we get the temporal relation between the electron and ion densities

. (12)

This relation assumes the current moves radially between the anode and the cathode of the thruster. By inserting (7)-(9) into (1)-(6) yields:

, (13)

, (14)

, (15)

(16)

, (17)

, (18)

, (19)

. (20)

For completeness, note that in the case of (12), the continuum equation for ions automatically holds true for Eqs. (13) - (20). To show the acceleration effect, it is convenient to proceed from specific characteristics to total properties such as total momentum or total kinetic energy of electron and ion fluids for the whole plasma cylinder. To do this, the limits for electron and ion fluids form the plasma medium. Let us define the total number of particles of the s-kind as

, (21)

Where *R _{e}* (t) is the limit for the electron fluid and

*R*(t) i is the limit for the ion fluid? For spatial homogeneous densities

_{i}*n*(t) and

_{e}*n*(t) we have

_{i}(22)

Which represents the law of particle conservation since there is no particle loss or particle-creation in the control volume and

where and .

For simplicity, set Then from (22) we get

. (23)

Calculate the total kinetic energy for electron and ion fluids as

(24)

And the total axial momentum as

. (25)

Equations (12) - (25) form the basis for most of the analysis to follow.

**Basic properties of rotating flow**

Now we consider the basic dynamical features of the profile (8) in cylindrical geometry. In this flow field, there appears an azimuthal component of the vorticity,

, (26)

which confirms that besides the azimuthal flow rotation in the plane z = const, there is also rotation in the plane *φ*= const. Since the velocity and electric fields given by Eqs. (8) And (9), respectively have the same form, there is now also an azimuthal magnetic field component, which leads to additional force components that can affect the flow dynamics. In order to demonstrate the influence of various factors on the acceleration of the flow one should rewrite Eq. (2) as

.

It is easy to see that for (8) and (26). If the electrical field has purely a potential origin, then.

It implies that the value of vorticity is defined only by the term.

However, at the initial stage, the dynamics of the flow is always determined by the cylindrical geometry of the system when electrical and magnetic fields play a weak role. To clarify this peculiarity, it is useful to consider the behavior of the corresponding flow for cold neutral gas with density *n* and velocity . Substitution of Eq. (8) into the corresponding continuity equation yields

,

And the force-free momentum equation

,

Yields the following set

(27)

(28)

(29)

(30)

This set of ordinary differential equations determine the primitive, temporal solution for force-free flow which may be useful for understanding the physical features of the full set (13)-(20). In particular, the solutions of Eqs. (28)- (30) can be expressed via a function *A(t)* :

(31)

Where *C*_{0} and *D*_{0} are some integration constants, and value

(32)

This underlines the temporal nonlocal character for dependencies corresponding to (8). It means that in real plasma flow, highly nonlinear oscillations of the radial velocities can occur without any noticeable change of the densities, azimuthal and axial velocities for the electron and ion fluids. This is because the temporal dependences of the values given by relations (31) depend only on time integrals of *A(t)* so that the oscillations in the latter are smoothed out. Such solutions do not exist in the linear limit since higher harmonics do not appear. As is seen from (31) and (32), here the radial and axial flow components are strongly coupled, especially for *A(t)* < 0, when there is flow compression in the radial direction. One can thus have axial acceleration in the asymmetric flow owing to energy transfer from the radial flow. On the other hand, for *A(t)* > 0 , the difference between the *D(t)* in the symmetric and asymmetric cases is insignificant, since *D(t) *decreases with time and there is no enhancement of axial flow.

It is instructive to consider the limit *C*_{0} = 0 when according to (31) there is no flow rotation and Eq. (27) has the following solution:

, (33)

Here, *A*(*t* = 0) = A . If A_{0}<0 , then Eq. (33) describes an approach to a singularity of flow. That is a well-known intrinsic feature of fluids especially in inviscid pressure less limit.

Now we consider the case of rotating flow when, then using the expression for *C(t) *from Eq. (31) we can rewrite (27) as

(34)

Differentiating Eq. (34) we get

From which with the help of (34) we obtain

(35)

This nonlinear ODE can be integrated numerically. As an illustration, we present here three cases of rotating primitive flow when corresponds to a non-zero derivative .

We = 0.1 put in all present computations sketched in **Figure. 2**. Here, curve 1 shows the evolution of a system for initially free from radial flow, curves 2 and 3 relate to an expanding and compressible flow. As is seen from these curves, the rotation eliminates the singularity and for large times ( t > 5) the evolution takes place in a similar way. We see that in all cases the radial flows remain relatively small. However, according to (31) and (32), this brings about a strong damping of *n(t)*, *C(t)* and *D(t)* . That is, here a temporal nonlocal effect is involved. However, when the radial velocity is initially negative (curves 3), the corresponding rotational *C(t)* and axial *D(t)* components, as well as the density n(t) , decreases much slower than in other cases. Such behavior might be accounted for by the fact that in all cases the dynamics of the free-flow involves only inertial acceleration, resulting in radial expansion of the fluid.

**Figure 2:** The evolution of A(t) for *A _{0}*= 0 (curve 1),

*A*= 1 (curve 2) and

_{0}*A*= -1(curve 3), under

_{0}*A*= 0.1. .

_{0}**Dynamics of a rotating plasma flow**

In this model, the acceleration effect is caused by the azimuthal electric field which comes about the variation of an external magnetic flux [Eq. (7)]. In our model, it is possible to go beyond the approach of quasi-neutrality [Eq. (12)]. These processes can lead to the generation of a local azimuthal time-dependent electric field [Eq. (12)], which may accelerate the rotation of the electron and ion fluids in different directions. As previously mentioned, the interactions of these flows with the external magnetic field propel the axial acceleration of the flow. In fact, here we get the process of redistribution of energy and momentum of flow in the external magnetic fields.

Thus, the objective is to find a parameter such as which makes the model successful. Such information may be drowned by solving a pure initial value problem for this rotating plasma flow describing the set (1)-(6). As an illustration of these possibilities, we present a few graphs corresponding to the simplest cases when the external magnetic field is the permanent, and there are no other initial electric fields in plasma flow: and . In all computations, we shall use . To avoid singular behavior that may invalidate our starting equations (1)-(6). We shall restrict our numerical examples to an initially expanding and slowly rotating plasma passing along the z-axis by setting and

. In **Figure. 3** the total axial momentum for electron and ion fluids are plotted when* B _{z0}*=1

*and*

*B*= -1, and in

_{r0}**Figure.4**. the same dependencies are presented for the case when

*B*=1

_{z0}*and*

*B*= 1. Namely these dependences illustrate what typically occurs with the flow dynamics when the value

_{r0}*B*changes with the opposite sign.

_{r0}**Figure 3:** The temporal dependence of *P _{ez}* (curve 1) and

*P*(curve 2) for

_{iz}*C*(0)= 10

_{i}^{-3},

*C*(0)= -10

_{e}^{-3}and

*B*= -1.

_{ro}**Figure 4:** The temporal dependence of *P _{ez}* (curve 1) and

*P*(curve 2) for

_{iz}*C*(0)= 10

_{i}^{-3},

*C*(0)= -10

_{e}^{-3}and

*B*= 1.

_{ro}As seen from these graphs, in all both cases we observe an acceleration of electron and ion component that reflects the coupling of electron and ion fluids. The initial conditions induce a redistribution of momentum to the axial degree of freedom from other degrees of freedoms in the rotating plasma flow. Here we observe the strong growth of total axial momentum in the electron scale of time. In particular, it means that there is a week influence due to the collisional phenomena on the momentum transfer. This is if the character electron time is less than the corresponding characteristic collision time.

We now examine whether the above presented results remain valid if electron and ion fluids are initially rotated in the same direction. **Figure.5**. illustrates when we set and all parameters coincide with the ones for **Figure. 3**. As is seen from the graphs of **Figure. 3**-**5**, maximum acceleration of ion fluid remains at the same level. Whereas the dependences of the electron component in **Figure. 3** and **5** are quite different from similar one in **Figure.4**. Thus, we come to the conclusion about a weak influence of initial velocity distribution and a strong effect of the external magnetic field on the processes of energy/momentum exchange.

**Figure 5:** The temporal dependence of *P _{ez}* (curve 1) and

*P*(curve 2) for

_{iz}*C*(0)= 10

_{i}^{-3},

*C*(0)= -10

_{e}^{-3}and

*B*= -1.

_{ro}So, we take the initial state which is distinct from the state plotted in **Figure. 3** only by *B _{z0}*= -1; the corresponding results are sketched in

**Figure. 6**. Here we see that the behavior is quite different from the dependences in

**Figure. 3**and

**4**. Moreover, in this case one can observe the increase of the acceleration effect both electron and ion components.

**Figure 6:** The temporal dependence of *P _{ez}* (curve 1) and

*P*(curve 2) for

_{iz}*C*(0)= 10

_{i}^{-3},

*C*(0)= -10

_{e}^{-3}and

*B*= -1. and

_{ro}*B*= -1.

_{zo}Summing up, all these results testify to the possibility of energy/momentum accumulation in the axial mode which is brought about by the energy/momentum transfer from other degrees of freedom due to the external magnetic fields. However, one can expect that such effects will be increased for external magnetic nonstationary fields [Eq. (6)].

From the comparison of **Figure. 3** and **4**, it follows that the change of sign for *B _{r0}* brings about the form of the observed dependences, the shape of the electron and ion dependences change over the course of time. It seems that these peculiarities are caused by not only asymmetrical rotation of electron and ion fluids for the same initial data. Such a behavior is made possible by the strong nonlinearity of the set (1)-(6). Thus, depending on the initial values, the system can evolve in many ways and this issue is required the further investigation.

Besides, the effect of intermodal exchange has been established in the hydrodynamic approach for a cold, neutral flow model of the cylindrical homogeneous plasma flow. Our study is based on using particular but exact nonlinear solutions of the electron and ion fluid equations. In fact, here we have the redistribution of energy/momentum between the macroscopic degrees of freedom in the cold plasma flow placed into the permanent magnetic fields. So we again would like to stress that we can significantly increase the acceleration effect by using non-stationary magnetic fields when the vortex component of the electric field has been produced.

**Concluding thoughts**

Results of this assessment implies that degrees of freedom of electrons and light ions in a plasma are capable of being changed based upon a weak magnetic field. The key is this capability is easily applicable to a Hall Thruster where the approach requires smaller chamber lengths to accelerate particles in the axial direction for thrust [4-8]. Results also provide limitations for the weak magnetic field which can be of a lower intensity than current systems. Such flows may be stable.

Other applications exist for other than space propulsion applications. Here, atmospheric disturbances such as tornadoes or even hurricanes may be altered by adjusting, assuming a large electromagnetic capability exists, to ameliorate weather conditions [26-28]. In the layers of the Earth's atmosphere contain a large number of charged particles under a vortex formation where the Earth’s magnetic, electric and non-inertial fields have dealt with gravity-heat and electrical processes of the Earth via the generation of geostrophic fluxes [26-31]. Thus, the present approach makes it possible to understand the processes of energy/momentum conversion in the atmosphere vortex entities of different scales [27-32].

Proceeding from the presented results for the dynamics of rotating plasma flows, we may also speculate about the similar effects for a gravitational field in the non-inertial reference systems. In a general case, we can represent the electric and magnetic fields in terms of a scalar and vector potentials as

That allows us to write the Lorentz force for the charge *q *moving with velocity with respect to an immobile reference system in the form

(37)

Now we consider the relation for gravitational force in a non-inertial system:

(38)

Where is the velocity of mass *m* with respect to moveable reference system rotating with respect to the fixed frame. Here is the velocity of rotation for moveable frame. As is seen from Eqs. (37) and (38), these forces have the same structure if we put . This point suggests that the processes of energy/momentum exchange and acceleration in rotating frames may come about by a similar way to the considered processes in the rotating plasma flow. We may venture a guess that such mechanisms may be realized in different astrophysical phenomena where one should also take into account the strong gravitational fields. Thus, the manifestations of energy/momentum exchange in different natural phenomena may be quite diverse, but there are some general features that are yet to be observed in almost all of these systems.

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