1. Collisions in Fully-Ionized Plasmas
We now look at a fully-ionized plasma. In this case all collisions are Coulomb collisions between charged particles.
It turns out that there is a major difference between like-particle collisions (ion-ion or electron-electron) and unlike-particle collisions (electron-ion or ion-electron)
Look at two identical particles making a collision
In a head-on collision the particles emerge with their velocities reversed so the particles simply interchange their orbits and the two guiding centers remain in the same traces.
The very worse case is a 90 collision in which the velocities are changed 90 in direction

2. Now, after the collision – the guiding centers have indeed shifted – but the “center of mass” of the guiding centers has remained steady. Now in collisions with neutrals all we cared about was the motion of the charged particle.
Here, we must consider both particles – and there’s
detailed balance.
For each ion that moves outward, there’s one that moves
inward.
Now the situation changes completely for unlike particle
collisions.
It turns out that the worst case is the 180 collisions. Here the particles emerge with their velocities reversed – for simplicity we’re looking at equal mass particles.
Since both particles must continue to gyrate in proper sense, the displacement of the guiding centers is in the same direction.
So unlike particle collisions give rise to diffusion.

3. Left: Schematic showing particle displacements in direct Coulomb
collisions between like species in a magnetized plasma. Right: Collisions
between unlike particles effectively displace guiding centers
Because of the mass disparity, electrons bounce off almost stationary
ions and execute a random walk of step length rL. In general, ions only move slightly, but very often. However, conservation of momentum implies that the diffusion rate for ions and electrons is the same (no charge separation, no electric fields).

4. The trajectory of a neutral particle in a partially ionized gas exhibits “straight-line" motion between abrupt atomic collisions.

5. The trajectory of a “test" charged particle (electron) in a partially
ionized gas exhibits continuous small-angle deflections or scatterings of its direction of motion. The largest deflections occur when a charged particle passes close to another charged particle.

6. Coulomb collisions
An ion nearing another will feel a repulsive force. What is the cross-section for a collision? The answer is ∞, since no matter how far apart the ions are, they will be deflected. However, we can define a cross-section for 90o scattering - cross-section for momentum transfer.
Sydney University

7. We can derive an approximate expression for the 90o scattering cross-section. The correct result is similar but the derivation is much more complicated, it takes into account the accumulated effect of many small angle collisions.

8. Assume ion remains at rest and the electron is incident with impact parameter, b, such that it is deflected 90o (b1=b2, v1=v2). The attractive force is given by:
F varies with time because r varies with time, so change in momentum is given by:

9. so get
when the integral is done properly the answer is:
The important point to note is that b∝v-2. If an electron is moving slowly, the force acts for a long time so the electron will experience a larger deflection than a fast electron at the same b.

10. The cross-section for deflections larger than 90o can be written as:
And so the collision frequency for Coulomb collisions of an electron with ions is:

11. Coulomb collisions
Coulomb collisions between free particles in a plasma is an elastic
process. Let us consider the Coulomb force between two test charges
q and Q:
This is a long range force and the cross-section for interaction of isolated charges is infinity! It is quite different from elastic “hard-sphere” encounters such as that which can occur between electrons and neutrals for example. In a plasma, however, the Debye shielding limits the range of the force so that an effective cross-section can be found. Nevertheless, because of the nature of the force, the most frequent Coulomb deflections result in only a small deviation of the particle path before it encounters another free charge. To produce an effective 90 degree scattering of the particle (and hence momentum
transfer) requires an accumulation of many such glancing collisions. The collision cross-section is then calculated by the statistical analysis of many such small-angle encounters.
University of Alaska, Antonius Otto

12. Consider the Coulomb force on an electron as it follows the unperturbed path shown in the picture, only the perpendicular component matters because the parallel component of the force reverses direction after q passes Q. Thus, = b/r or
where b is the impact parameter for the interaction. Since x (the
Parallel coordinate) changes with time, we integrate along the path to
obtain the net perpendicular impulse delivered to q

13. Now
so that
We consider a statistical average over a random distribution of such small
angle collisions. For a random walk with step length s, the total
displacement after N steps is (i.e )
where N is the number of steps. The total change in velocity is thus

14. Now integrate over the range of impact parameters b to estimate the number
of glancing collisions in time t. Small angle collisions are much less
likely because of the geometrical effect
We combine the three equations above and integrate over impact
parameter:
bmin is the closest approach that satisfies the small deflection
hypothesis. We obtain this be setting

15. Outside D the charge Q is not felt. We thus take bmax =D and
ln is called the Coulomb logarithm and is a slowly varying function of
electron density and temperature. For fusion plasma, ln  One
usually sets ln = 10 in quantitative estimations.

16. For electron-ion encounters, q = -e and Q = Ze so
We are finally in a position to find the elapsed time necessary for a net
90 degree deflection, i.e.
and
For electron-ion encounters, q = -e and Q = Ze so
and ei = nieiv implies that

17. Derivation Review Perpendicular impulse  1/vb Angular deflection
Random walk to scatter one radian
Integrate over
The dependence has very important ramifications. A
high temperature plasma is essentially collisionless. This means that
plasma resistance decreases as temperature increases. In some
circumstances populations of particles can be continually accelerated,
losing energy only through synchrotron radiation (for example
runaway electrons in a tokamak).

18. Sketch of the collisional drag Fc acting on electrons as a function of their velocity vd for E > ED. The black arrows indicate the overall acceleration or deceleration.

19. Melting damage to the upper inner wall of JET, thought to be caused by run-away electrons.

20. Energy transfer in electron-ion collisions
A pervading theme in plasma physics is me  mi. This has consequences
for collisions between the species in that we expect very little energy
Transfer between the species. To illustrate this, consider such a collision
in the centre-of-mass frame (a direct hit).

21. Collision between ion and electron in center of mass frame
eliminate V, V0:

22. Now translate to frame in which ion M is at rest (initially)
Now translate to frame in which ion M is at rest (initially). In this frame the initial electron energy is
and the final ion energy is
Their ratio is given by
and thus

23. For glancing collisions the energy transfer between ions and electrons is even less.
Coulomb collisions result in very poor energy transfer between electrons
and ions. The rate of energy transfer is roughly (me/mi) slower than the
e-i collision frequency. On the other hand, energy transfer rate and
collision frequency are the same for collisions between ions
ii  ei(me/mi) :
That is,

24. Coulomb Cross section for Momentum Exchange
Scattering of momentum reduces the momentum of a stream of particles
and is therefore generates resistance for a stream particles. To measure
the resistance we need the total cross section for the momentum
scattering.
Assume scattering of a particle with mass m , charge q , and velocity v
by a particle with mass and charge q0 . The impact parameter
is b .
Antonius Otto

25. Mechanics:
The momentum along x after the scattering is
such that the momentum change is
Let N be the number of particles per time unit and unit area:
Then particles are scattered into the range

26. Definition: Differential cross section for momentum exchange

27. total cross section:
with
and we obtain

28. and for
Finally, we can express  through the scattering parameters by noting
that for small values of  we have
such that
Here, the expression
is called the Coulomb logarithm.

29. Note that p,tot  electrical resistance
For
Conclusion: The simple model of Coulomb scattering yields an
inconsistency. The total cross section diverges through the contribution
of large numbers of particle with large impact parameters. However,
at distance larger than the Debye length the coulomb potential is
shielded.
Let us also consider a hydrogen plasma with

30. => Coulomb logarithm is the logarithm of the plasma parameter!
No coincidence: The plasma parameter (and powers thereof) is the only
possibility to create a dimensionless parameter that is a function of
m , e , n , and T .

31. Collision frequency
The collision frequency is equal to the flux of particles vn0 multiplied
with the total cross section p,tot :
Consider a Maxwell distribution function:

32. Integrating over velocity space yields the average
such that
It is interesting to compare collision and plasma frequency:
Binary collisions are less important than collective plasma effects!!

33. Collisions in Plasmas 3.1 Binary collisions between charged particles
Hutchinson

34. Figure 3.1: Geometry of the collision orbit

38. 3.1.1 Frames of Reference

39. 3.1.2 Scattering Angle
Figure 3.2: Relation between 1 and  .

42. Figure 3.3: Collisions viewed in Center of Mass and Laboratory frame.

43. 3.2 Differential Cross-Section for Scattering by Angle
Rutherford Cross-Section

45. Figure 3.4: Scattering angle and solid angle relationship.

46. Figure 3.5: Annular volume corresponding to db.

50. 2 Coulomb collisions
H. J. de Blank
PLASMA PHYSICS Lecture Notes

56. A Appendix: Coulomb collisions
H. J. de Blank
PLASMA PHYSICS Lecture Notes

59. Figure 38: Motion around a fixed center of force

62. Coulomb Collisions*
*Ref. Jackson Classical Electrodynamics, Chapter 13
We will now look at small-angle coulomb scatterings since these are what is responsible for the resistivity of a plasma.
We consider a particle with charge q1 and initial momentum mvo scattered by a fixed particle of charge q2.
We assume that the impact parameter is large enough that the angle of deflection of
particle 1 is small
The geometry is as shown.

63. Now for x << 1 we have:
Now so and is the force acting on particle 1.
From the diagram you can see that
Now we can also write using the fact that the angular momentum of particle 1 about 2 is given by so or

64. Now taking electrons and singly charged ions we can write:
Then:
Now taking electrons and singly charged ions we can write:
We recall that the differential scattering crossection is defined by: so
Note the exact Rutherford scattering crossection is

65. But using we have
Now, from what we know of plasma physics so far we suspect that plasma effects – i.e. Debye shielding may turn out to alter this result somewhat.
For impact parameters the order of or greater than the Debye length, the potential falls off rapidly so the scattering angle will tend to vanish much more rapidly with increasing impact parameter than we have indicated.
So the differential scattering cross section should flatten out rather than increasing with
x-4. Therefore, we put in a cutoff:

66. To calculate xmin we let b = D in the expression for x.
and letting
There is also a maximum value for x.
Quantum mechanically

67. Summary 1. Want to calculate ei [i.e. shielded Coulomb collisions].
where x is the scattering x = x(b). 3. 4.
where

68. Scattering Cross Section
All these land here
N0: The number of particles incident on the target foil per unit area per unit time.
Any incident particles entering with impact parameter b and b+db will scatter to the angle q and q-dq.
In other words, they scatter into the solid angle dW (=2psinqdq).
So the number of particles scattered into the solid angle dW per unit time is 2pN0bdb.
PHYS 3446, Fall 2006
Jae Yu

69. Scattering Cross Section
For a central potential
Such as Coulomb potential
Which has spherical symmetry
The scattering center presents an effective transverse cross-sectional area of
For the particles to scatter into q and q+dq

70. Scattering Cross Section
In more generalized cases, Ds depends on both q & f.
With a spherical symmetry, f can be integrated out:
Why negative?
Since the deflection and change of b are in opposite direction!!
What is the dimension of the differential cross section?
Differential
Cross Section
reorganize
Area!!

71. Scattering Cross Section
For a central potential, measuring the yield as a function of q, or differential cross section, is equivalent to measuring the entire effect of the scattering
So what is the physical meaning of the differential cross section?
Measurement of yield as a function of specific experimental variable
This is equivalent to measuring the probability of occurrence of a physical process in a specific kinematic phase space
Cross sections are measured in the unit of barns:
Where does this come from?
Cross sectional area of a typical nucleus!

72. Total Cross Section
Total cross section is the integration of the differential cross section over the entire solid angle, W:
Total cross section represents the effective size of the scattering center at all possible impact parameter

73. Cross Section of Rutherford Scattering
The impact parameter in Rutherford scattering is
Thus,
Differential cross section of Rutherford scattering is

74. Rutherford Scattering Cross Section
Let’s plug in the numbers
ZAu=79
ZHe=2
For E=10 keV
Differential cross section of Rutherford scattering

75. Total X-Section of Rutherford Scattering
To obtain the total cross section of Rutherford scattering, one integrates the differential cross section over all q:
What is the result of this integration?
Infinity!!
Does this make sense?
Yes
Why?
Since the Coulomb force’s range is infinite.
Is this physically meaningful? No
What would be the sensible thing to do?
Integrate to a cut-off angle since after certain distance the force is too weak to impact the scattering. (q=q0>0)

76. Measuring Cross Sections
Rutherford scattering experiment
Used a collimated beam of a particles emitted from Radon
A thin Au foil target
A scintillating glass screen with ZnS phosphor deposit
Telescope to view limited area of solid angle
Telescope only need to move along q not f. Why?
Due to the spherical symmetry, scattering only depends on q not f.

77. Measuring Cross Sections
With the flux of N0 per unit area per second
Any a particles in b and b+db will be scattered into q and q-dq
The telescope aperture limits the measurable area to
How could they have increased the rate of measurement?
By constructing an annular telescope
By how much would it increase?
2p/df

78. Measuring Cross Sections
Fraction of incident particles approaching the target in the small area Ds=bdfdb at impact parameter b is –dn/N0.
dn particles scatter into R2dW, the aperture of the telescope
This ratio is the same as
The sum of Ds over all N nuclear centers throughout the foil divided by the total area (S) of the foil.
Probability for incident particles to enter within the N areas of the annular rings and subsequently scatter into the telescope aperture
So this ratio can be expressed as

79. Measuring Cross Sections
For a foil with thickness t, mass density r, atomic weight A:
Since from what we have learned previously
The number of a scattered into the detector angle (q,f) is
A0: Avogadro’s number of atoms per mol

80. Measuring Cross Sections
Detector acceptance
Number of detected particles
Projectile particle flux
Density of the target particles
Scattering cross section
This is a general expression for any scattering process, independent of the existence of theory
This gives an observed counts per second

81. Coulomb collisions
An ion nearing another will feel a repulsive force. What is the
cross-section for a collision? The answer is ∞, since no matter how far
apart the ions are, they will be deflected. However we can define a
cross-section for 90o scattering - cross-section for momentum transfer.
We can derive an approximate expression for the 90o scattering
cross-section. The correct result is similar but the derivation is much
more complicated, it takes into account the accumulated effect of
many small angle collisions.
University of Sydney

83. Assume ion remains at rest and the electron is incident with impact
parameter, b, such that it is deflected 90o (b1=b2, v1=v2). The
attractive force is given by:
F varies with time because r varies with time, so change in momentum
is given by:

84. So we get:
when the integral is done properly the answer is:
The important point to note is that b∝v-2. If an electron is moving
slowly, the force acts for a long time so the electron will experience a
larger deflection than a fast electron at the same b.

85. The cross-section for deflections larger than 90o can be written as:
And so the collision frequency for Coulomb collisions of an electron
with ions is: