## Brazilian Journal of Physics

##
*On-line version* ISSN 1678-4448

### Braz. J. Phys. vol. 27 n. 4 São Paulo Dec. 1997

#### http://dx.doi.org/10.1590/S0103-97331997000400011

**Inverse Dynamics in the Classical Fermi Accelerator **

M.S. Hussein^{1}, and M.P. Pato

*Nuclear Theory and Elementary Particle Phenomenology Group,*

*Departamento de Física Nuclear, Instituto de Física,*

*Universidade de São Paulo. C.P. 66318, 05389-970, São Paulo, SP, Brazil *

V. Kharchenko^{2}

*Institute for Theoretical Atomic and Molecular Physics at the*

*Harvard-Smithsonian Center for Astrophysics*

*60 Garden Street*

*Cambridge, Massachusetts 02138 U.S.A.*

**Received June 22, 1997 **

The motion of a particle constrained to move between two walls one of which is moveable is solved. We determine analytically the effective forces that act on the particle or on the moveable wall. The quantal version of the solution is briefly discussed.

**I. Introduction**

Classical Mechanics text books discuss friction forces without paying much attention to the dvnamics behind their origin. It would be useful for didatical purposes, to develop simple models that allows one to "derive'' friction forces and thus enables one to discuss their properties.

In this paper we fully solve a simple one-dimentional problem for this purpose. The problem at hand is that of the motion of a particle of mass m constrained within a region bounded by two walls one with infinite mass and the other with arbitrary mass M > m.

When the wall with mass M is oscillating the system is called a Fermi Accelerator [1] and has been investigated in the past by Ulam [2]. Usually Ulam's model has been used for he investigation of the stochastic acceleration of the light particles in collisions with the moving heavy obJects [2-5]. In this paper we study a simpler problem of a free movable wall. The model can be schematized as in Fig. 1. In contrast to the Fermi accelerator, we study the inverse process, where the kinetic energy of the light particle is ransferred to the heavy particle - the movable wall. Upon hitting the fixed wall the particle loses momentum but not energy whereas collision with the movable wall allows for loss of momentum and energy. Our model is relevant to studies involvin the confinement of ultracold neutrons in bottles [6]. Further, it is analytically fully soluble. In Section II, for a given value z º m/M, we solve, fully the problem and obtain the value of the velocities of the particle, n_{n}, and the movable wall, V_{n}, after their n^{th} collision. In Section III, we discuss the effective force that acts on the light particle due to the collisions with the wall. In Section IV we give a brief discussion of the quantum mechanicaI solution recently obtained by Hussein and Kharchenko [7]. Finally, in Section V we present our concluding remarks.

Figure 1. A schematic figure showing the Inverse Fermi Accelerator.

**II. Exact solution of the Inverse Fermi Accelerator**

The conservation of momentum and energy after the n collision is given by the following recursive formula

The solution of the above equations can be written in a matrix form

where we have introduced the parameter

Recursion relation given by Eq.2 allows to evaluate the velocities of the light and heavy particles after n-th collisions, if their initial velocities are known:

Momentum and energy transfer between heavy and light sub-systems is stopped after some number of collisions. i. e. there is a critical n, n_{c}, after which the particle always lags behind the now moving wall.

To obtain a closed expression for V_{n} and n_{n} we first recognize that Eq.(2) can be thought of as an evolution equation for a two-dimensional velocity vector which we call

This vector is not conserved, neither its length nor its direction, and the velocity evolution matrix describes these changes.

It is possible however, to define a constant-length vector in the phase space form the energy conservation equation Eq.1b. vis [8]

Clearly

which is a constant. In this case the collisional evolution of the system is described by the phase F_{n} of the _{n} vector

Thus _{n} evolves in a circle and the matrix that relates the components and to and is an elementary rotation

Call

Thus

which is the rotation matrix in two dimensions through angle a. Clearly, after n collisions the velocity evolution matrix is given by B^{n}

Thus

Or finally the velocity vector projections from the Eq.(5) satisfy the eliptic equations

and

where the initial phase angle F_{0} can be calculated via the initial velocities of the Eq.(4). The magnitude of the total phase F_{n} = na+ F_{0} is restricted: |F_{n}| £ and it allows the evaluation of the maximum number of collisions N_{max}, for a system with arbitrary initial conditions and mass ratio z = m/M. Indeed, according to Eq.(14)

where the function Int[x] gives the greatest integer less than or equal to x. The evolution of velocities, Eq.(14), is more simple in the case of zero initial velocity of the moveable wall, V_{0} = 0. The initial phase F_{0} = O and

The total number of collisions n = n^{(0)}_{c} between particle and wall is restricted by the conditions V_{n} £ n_{n}, or tg(n_{c}^{(0)}) £ 1/z^{1/2}. The last inequality can be written as the restriction of the total angle of rotation in the phase space na:

For the adiabatic limit z = m/M << 1 the elementary phase angle a is very small (a 2z^{1/2}), F_{nc(0)} and critical value n_{c}^{(0)} can be estimated as

To verify the above findings, we have numerically solved Eq.(2), taking for initial conditions n(0) = n_{0} = 1, V(0) = 0, r(0) = 0, R(0) = R_{0} = 1 (see Fig. 1). The results are shown in Figs. 2 and 3 for z = 4 ×10^{-2} and 10^{-4}, respectively. The value of n_{c} in Figs. 2 is 5, close to 4. In Fig. 3, we have n_{c}^{(0)} 78. compared to 78.5. Further, Fig. 3 shows a rather smooth function of time. The agreement with the analytical results, Eq.(19), is excellent. This would allow the extraction of an effective friction force which we discuss in the following section.

Figure 2. The velocities n_{n} and V_{n} vs. t for z = 4 ×10^{-2}, m = n_{0} = R_{0} = 1.

Figure 3. Same as Fig.2 for z = 10^{-4}.

For a system with arbitrary initial velocities the critical (or total) number of collisons between particle and moveable wall n_{c} is defined as a maximal value of n satisfying velocity conditions n_{n} ³ V_{n}, or tg F_{n} £ :

For the adiabatic limit z = m/M £ 1 the elementary phase angle a is very small (a 2z^{1/2} ), and one can derive the asymptotic formula

It is important to note, that the intial phase angle F_{0} can be positive or negative, depending on the relative orientation of the particle and the wall velocities. If the wall initially moves to the left, F_{0} < O and the number of collisions n_{s}, needed to stop the wall or to change the wall velocity direction is

where the initial kinetic energies of the light particle and the moveable wall are denoted by k_{0} and K_{0} respectively. The situation during these n_{s}, collisions can be described as an acceleration of the particle as the kinetic energy of the wall is transferred to it until the wall comes to a halt, followed by the inverse Fermi acceleration when the particle losses energy. The critical number of collisions for arbitrary initial velocities is

where n^{(-)}_{c} and n^{(+)}_{c} are critical number of collisions for the initial movable wall velocity towards and away from the stationary wall. Phase space diagrams for the different initial conditions are shown in the Fig. 4. From the Eqs. (22), (23) it is not difficult to extract the collisionless condition n^{(+)} = (n^{(0)}_{c} -n_{s}) £ 0, that is identical to the velocity relation V_{0} ³ n_{0}. According to Eq. (22) the maximal number of the collisions nededed to stop the wall is n_{s} n^{(0)}_{c} and thus n^{(-)}_{c} = 2n^{(0)}_{c} . This result shows a good agreement with our general estimate of the maximal number of collisions from Eq.(16): N_{max} = , which is given for the particular case of asymptotically small value of z. The method of finite rotation in phase space, developed in his Section, provides the exact evaluation of the velocity evolution matrix. Natural generalization of this method for the completely quantal Fermi accelerator system allows also to find the exact quantum solution, as has been shown in [7].

Figure 4. The phase space diagram for the positive (a) and negative (b) velocity projection of moveable wall.

**III. The particle-wall effective force**

In this section the particle wall effective force is studied for the strong adiabatic condition, when the parameter z << 1 and elementary rotational angle a 2z^{1/2} is very small. The critical number of collisions in this case is very large (see Eqs.(19),(23)) and for the description of the velocity evolution of both the particle and the wall we can use a quasi-continuous variable n related with the time

We write for the time variation of the kinetic energy of m the following rate equation

where F_{ef}, represents the effective force felt by m due to its collisions with the moveable wall. Clearly, from conservation of total energy,

Since, from Eq. (17)

Or with Eq. (24)

thus

and

which gives

or

Now R_{n}(t) can be obtained from Eq.(32) by simple integration. A closed expression is obtained by setting az^{-1/2} ~ 2 which is an excellent approximation for << 1. We thus find

Putting things together, we finally obtain for the effective force the following expression

or

and

The above functions peak at n_{0}/, z^{1/2}n_{0}/and R_{0}/z^{1/2}n_{0} respectively. Before we end this section, we give in the following the expression for the acceleration of the movable wall, d^{2}R/dt^{2}. From Eq.(34), we find

The numerically generated effective force is shown as functions of n_{0}-n, V and t, in Figs. 5, 6 and 7, respectively, for z = 10^{-4}. The agreement with our analytical formulae, Eqs. (35), (36) and (37) is excellent. We should mention, however, that Eqs. (35-38) are approximate formulae valid in the limit of a very large number of collisions and at times shorter than the time, t_{c}, at which the velocities attain their terminal values. Clearly, at longer times the acceleration is identically zero. Before we end this section, we comment on the difference between the effective "friction" force, given by m and the acceleration force M. Whereas the movable wall of mass M receives energy through energy - and momentum-conserving collisions with m, the particle suffers also momentum-nonconserving collisions with the fixed wall. In each of these collisions, say the n^{th} one, a quantity of momentum, 2mn_{n}, is lost to the fixed wall. This is basically the reason why F_{ef}/m, Eq.(37), is qualitativelv different from of Eq.(38).

Figure 5. The friction force corresponding to the case of z = 10^{-4} (Fig.3).

Figure 6. Same as Fig.5 but vs. V.

Figure 7. Same as Fig.6 but vs. time.

**IV. Semiquantal treatment of the inverse Fermi accelerator**

In a recent work [7] two of us soived the problem of the inverse Fermi accelerator quantum mechanically for the light and heavy particles. The solution was obtained for different limits: the semi-quantal, the full Born-Oppenheimer and the exact solutions were presented. It is instructive to compare the classical results obtained in the present paper. with the semi-quantal solution. where the moving wall is treated classically while the particle quantum mechanically. The quantized motion of the particle is fully described by the normalized wave function

n = 1,2 ....

The eigenenergies, e_{1} are

The classical "Hamiltonian" that describes the motion of the wall is accordingly given by

It is clear that there are infinite number of Hamiltonians corresponding to the infinite number of eigenstates of m described by (39). From the equation of motion follows

On the other hand, the conservation of total energy gives

Thus

With Eq.(44), Eq.(42) becomes

Notice, that all reference to quantum mechanics in (45) is contained in the definition of the terminal velocity V_{¥}, Eq. (44). We see from (38) and (45) an apparent equality between the classical and semiquantal treatments of the inverse Fermi accelerator. There is, however, an important difference between the two. As we have discussed in Section III, Eq.(38) is valid only at times shorter than the limiting time t_{c}. On the other hand, when treated quantum mechanically, the particle will have continuous distribution of velocities. Accordingly the interaction between wall and the particle may be considered "continuous'' thus making Eq.(45) valid for all times.

**V. Conclusions**

In this paper the classical solution of the inverse Fermi accelerator is presented in details. The effective "friction" force that acts on the particle due to its collisions with the moveable wall in derived. A semiquantal solution of the problem is also presented. The classical and quantal accelerating forces that act on the movable wall were found to be identical at times shorter than the critical time at which classically the particle and wall attain their terminal velocities.

**Aknowledgement**

This work was partially supported by the National Science Foundation through a grant for the Institute for Theoretical Atomic and Molecular Physics at Harvard University and Smithsonian Astrophysical Observatory.

**References**

- 1.
- E. Fermi. Phys. Rev.
**75**, 1169 (1949). [ Links ] - 2.
- S. Ulam,
*Proc. 4*3, 315 (Berkeley-Los Angeles, 1961).^{th}Berkeley Symposium on Mathematics and Probability [ Links ] - 3.
- A.J. Lichtenberg and A.M. Lieberman,
*Regular and Chaotic dynamics*, Springer, Berlin, 1992. [ Links ] - 4.
- G. M. Zaslavsky,
*Chaos in dynamic systems*, Harwood Academic Publishers, New York, 1985. [ Links ] - 5.
- J. V. Jose and K. Cordery, Phys. Rev. Lett.,
**56**, 290 (1986). [ Links ] - 6.
- W. Mampe, P. Ageron. C. Bates, J. M. Pendlebury and A. Steyerl, Phys. Rev. Lett.
**63**, 593 (1989). [ Links ] - 7.
- M.S. Hussein and V. Kharchenko, Ann. Phys. (NY) (1995), in press. [ Links ]
- 8.
- R.H. Romer, Am. J. Phys.
**35**, 862 (1967).

^{1} Supported in part by CNPq (Brazil). e-mail: hussein@if.usp.br

^{2} Supported by the National Science Foundation