ESS 200C Lecture 13 The Earth’s Ionosphere

1. ESS 200CLecture 13The Earth’s Ionosphere

2. Ionospheric studies • The radiation from the Sun at short wave lengths causes photo ionization of the atmosphere resulting in a partially ionized region called the ionosphere. • Guglielmo Marconi’s demonstration of long distance radio communication in 1901 started studies of the ionosphere. • Arthur Kennelly and Oliver Heaviside independently in 1902 postulated an ionized atmosphere to account for radio transmissions. (Kennelly-Heavyside layer is now called the E-layer). • Larmor (1924) developed a theory of reflection of radio waves from an ionized region. • Breit and Tuve in 1926 developed a method for probing the ionosphere by measuring the round-trip for reflected radio waves.

3. The extent of the ionosphere • There are ions and electrons at all altitudes in the atmosphere. • Below about 60km the charged particles do not play an important part in determining the chemical or physical properties of the atmosphere. • Identification of ionospheric layers is related to inflection points in the vertical density profile.

5. Diurnal and solar cycle variation in the ionospheric density profile. In general densities are larger during solar maximum than during solar minimum. The D and F1 regions disappear at night. The E and F2 regions become much weaker. The topside ionosphere is basically an extension of the magnetosphere.

6. Composition of the dayside ionosphere under solar minimum conditions. At low altitudes the major ions are O2+ and NO+ Near the F2 peak it changes to O+ The topside ionosphere becomes H+ dominant.

7. For practical purposes the ionosphere can be thought of as quasi-neutral (the net charge is practically zero in each volume element with enough particles). • The ionosphere is formed by ionization of the three main atmospheric constituents N2, O2, and O. • The primary ionization mechanism is photoionization by extreme ultraviolet (EUV) and X-ray radiation. • In some areas ionization by particle precipitation is also important. • The ionization process is followed by a series of chemical reactions which produce other ions. • Recombination removes free charges and transforms the ions to neutral particles.

8. Neutral density exceeds the ion density below about 500 km.

9. Let the photon flux per unit frequency be The change in the flux due to absorption by the neutral gas in a distance ds is where n(z) is the neutral gas density, is the frequency dependent photo absorption cross section (m2), and ds is the path length element in the direction of the optical radiation. (Assuming there are no local sources or sinks of ionizing radiation.) (where is the zenith angle of the incoming solar radiation. The altitude dependence of the solar radiation flux becomes where is the incident photon intensity per unit frequency. is called the optical depth. There is usually more than one atmospheric constituent attenuating the photons each of which has its own cross section. Ionization profile

10. The density (ns) of the neutral upper atmosphere usually obeys a hydrostatic equation where m is the molecular or atomic mass, g is the acceleration due to gravity, z is the altitude and p=nkT is the thermal pressure. If the temperature T is assumed independent of z, this equation has the exponential solution where is the scale height of the gas, and n0 is the density at the reference altitude z0. For this case For multiple species The optical depth increases exponentially with decreasing altitude. In the thermosphere solar radiation is absorbed mainly via ionization processes. Let us assume that Each absorbed photon creates a new electron-ion pair therefore the electron production is where Si is the total electron production rate (particles cm-3s -1).

11. Substituting for n and gives The altitude of maximum ionization can be obtained by looking for extremes in this equation by calculating This gives Choose z0as the altitude of maximum ionization for perpendicular solar radiation This gives where This is the Chapman ionization function. The maximum rate of ionization is given by If we further assume that the main loss process is ion-electron recombination with a coefficient a and assume that the recombination rate is Finally if we assume local equilibrium between production and loss we get

12. The vertical profile in a simple Chapman layer is The E and F1 regions are essentially Chapman layers Additional production, transport and loss processes are necessary to understand the D and F2 regions.

13. The D Region • The most complex and least understood layer in the ionosphere. • The primary source of ionization in the D region is ionization by solar X-rays which ionize both N2 and O2 • Lyman-a ionization of the NO molecule. • Precipitating magnetospheric electrons may also be important. • Initial positive ions are N2+, O2+ and NO+ • The primary positive ions are O2+ and NO+ • The most common negative ion is NO3- • The first step in making a negative ion is

14. The E Region • Essentially a Chapman layer formed by EUV ionization • The main ions are O2+ and NO+ • Although nitrogen (N2) molecules are the most common in the atmosphere N2+ is not common because it is unstable to charge exchange. For example • Oxygen ions are removed by the following reactions

15. The F1 Region • Essentially a Chapman layer. • The ionizing radiation is EUV at <91nm. • It is basically absorbed in this region and does not penetrate into the E region. • The principal initial ion is O+. • O+ recombines in a two step process because recombination of oxygen is slow. • First atom ion interchange takes place • This is followed by dissociative recombination of O2+ and NO+

16. The F2 Region • The major ion is O+. • This region cannot be a Chapman layer since the atmosphere above the F1 region is optically thin to most ionizing radiation. • This region is formed by an interplay between ion sources, sinks and ambipolar diffusion. • The dominant ionization source is photoionization of atomic oxygen • The oxygen ions are lost by a two step process • First atom-ion interchange • Dissociative recombination • The peak forms because the loss rate falls off more rapidly than the production rate. • The density falls off at higher altitudes because of diffusion- no longer in local photochemical equilibrium.

17. Ionospheric conductance • The dense regions of the ionosphere (the D, E and F regions) contain concentrations of free electrons and ions. These mobile charges make the ionosphere highly conducting. • Electrical currents can be generated in the ionosphere. • The ionosphere is collisional. Assume that it has an electric field but for now no magnetic field. The ion and electron equations of motion will be where is the ion neutral collision frequency and is the electron neutral collision frequency. • For this simple case the current will be related to the electric field by where is a scalar conductivity. • If there is a magnetic field there are magnetic field terms in the momentum equation. In a coordinate system with along the z-axis the conductivity becomes a tensor.

18. Specific conductivity – along the magnetic field • Pedersen conductivity – in the direction of the applied electric field • Hall conductivity – in the direction perpendicular to the applied field where and are the total electron and ion momentum transfer collision frequencies and and are the electron and ion gyrofrequencies. • The Hall conductivity is important only in the D and E regions. • The specific conductivity is very important for magnetosphere and ionosphere physics. If all field lines would be equipotentials. • Electric fields generated in the ionosphere (magnetosphere) would map along magnetic field lines into the magnetosphere (ionosphere)

19. Assume a generalized Ohm’s law of the form and that • The total current density in the ionosphere is where and refer to perpendicular and parallel to the magnetic field. • Space plasmas are quasi-neutral so where • The current continuity equation can be written where is along the magnetic field. • Integrate along the magnetic field line from the bottom of the ionosphere to infinity. Since the field lines are nearly equipotentials we can write where the perpendicular height integrated conductivity tensor is

20. Ionospheric Pedersen conductance viewed from dusk. Note the large day-night asymmetry. This results from of ionization by solar EUV radiation.

21. Ionospheric Hall and Pedersen conductance from a simulation of the magnetosphere during a prolonged period with southward IMF. • The white lines show the ionospheric convection pattern. • Precipitation from the magnetosphere enhances both the Hall and Pedersen conductances at night. Pedersen Conductance Hall Conductance

22. Field aligned currents from the simulation in the previous calculation. Cold colors indicate currents away from the Earth and hot colors indicate currents toward the earth. The high latitude currents are caused by the vorticity of polar convection cells.

23. Within the high latitude magnetosphere (auroral zone and polar cap) plasmas undergo a circulation cycle. • At the highest latitudes the geomagnetic field lines are “open” in that only one end is connected to the Earth. • Ionospheric plasma expands freely in the flux tube as if the outer boundary condition was zero pressure. • For H+ and He+ plasma enters the flux tube at a rate limited by the source. • The net result is a flux of low density supersonic cold light ions into the lobes. • The surprising part is that comparable O+ fluxes also are observed.