………………………………………………………..(Ionosphere Layers)
CONTENTS
IONOSPHERE DENSITIES
IONOSPHERE CHARGE
IONOSPHERE COMPOSITION
IONOSPHERE ELECTRON ACTIONS
IONOSPHERE ELECTRIC CURRENT PROBLEMS
IONOSPHERE EFFECTS ON EM RADIATION
IONOSPHERE CHANGES AT NIGHT
MEGALIGHTNING DESTROYED COLUMBIA?
IONOSPHERE DENSITIES
Here's a simple table showing the approximate densities for each layer of the ionosphere:
Layer -- Height (km) -- DENSITY: Negative (cm⁻³); Positive (cm⁻³); Neutral (cm⁻³)
D ---------- 48-90 --------------- 10² - 10⁴ ------------- 10² - 10⁴ ----------- 10¹³ - 10¹⁵
E ---------- 90-150 -------------- 10⁵ ------------------- 10⁵ ----------------- 10¹¹ - 10¹³
F1 -------- 150-220 ------------- 10⁵ - 10⁶ ------------- 10⁵ - 10⁶ ------------ 10⁹ - 10¹¹
F2 -------- 220-500+ ------------ 10⁶ ------------------- 10⁶ ------------------ 10⁷ - 10⁹
Note: These values are approximate and can vary significantly based on time of day, season, solar activity, and latitude. The negative density primarily refers to electrons, while the positive density refers to ions. The neutral density decreases with altitude, while ionization generally increases.
IONOSPHERE CHARGE
None of the ionospheric layers have a predominantly positive or negative charge. The ionosphere maintains quasi-neutrality throughout its layers, meaning the number of positively charged ions is approximately equal to the number of negatively charged electrons1. This balance of charges is a fundamental characteristic of ionospheric plasma.
1. https://link.springer.com/referenceworkentry/10.1007/1-4020-4520-4_194
The electrons (from the solar wind) that cause auroras do not reach the ground. Instead, they collide with atoms and molecules in Earth's upper atmosphere, typically at an altitude of about 60-200 miles (100-320 kilometers) above the Earth's surface1,3. When these high-energy electrons interact with oxygen and nitrogen atoms in the ionosphere, they transfer their energy, causing the atoms to become excited4. As these excited atoms return to their normal state, they emit photons, creating the colorful light displays we see as auroras4.
After the collisions, the electrons lose most of their energy. Some of the lower-energy secondary electrons that result from these collisions may:
_Continue to interact with other atmospheric particles, causing further excitation and light emission.
_Be scattered in various directions, including back up towards space1.
_Gradually lose more energy through subsequent collisions and eventually become part of the ionosphere.
The electrons do not penetrate further down into the lower atmosphere or reach the Earth's surface due to the increasing density of the atmosphere at lower altitudes, which effectively stops their downward motion3.
1. https://www.sciencedaily.com/releases/2015/10/151007185043.htm
2. https://www.energy.gov/science/fes/articles/source-aurora-borealis-electrons-surfing-alfven-waves
3. https://phys.org/news/2018-02-scientists-electron-dynamics-northern.html
4. https://www.space.com/aurora-origin-mystery-solved-by-electrons
IONOSPHERE COMPOSITION
The D, E, and F layers of the ionosphere are composed of different ions, atoms, and molecules:
D Layer (48-90 km)
Dominant ions: NO+ and O2+ (2)
Ionization source: Lyman series-alpha hydrogen radiation ionizing nitric oxide (NO)(8)
Other molecules: N2 and O2 (ionized during solar flares)(8)
E Layer (100-150 km)
Composition: Molecular ions O2+ and NO+, and atomic ions O+ (1)
Ionization source: Soft X-ray (1-10 nm) and far ultraviolet (UV) solar radiation ionizing molecular species(1)
F Layer (150-500+ km)
F1 Layer (lower part, 150-220 km):
Composition: Mixture of molecular ions O2+ and NO+, and atomic ions O+ (1)
F2 Layer (upper part, above 220 km):
The F layer is primarily ionized by extreme ultraviolet (UV) radiation in the 10-100 nm range, which ionizes atomic oxygen(8).
IONOSPHERE ELECTRON ACTIONS
The electrons from the solar wind that enter Earth's upper atmosphere do not directly push other electrons out of the atmosphere. Instead, the process is more complex and involves several mechanisms:
Trapping and redirection: Earth's magnetic field captures many of the incoming solar wind electrons, trapping them in the magnetosphere and redirecting them towards the polar regions1.
Energy transfer: When these high-energy electrons collide with atoms and molecules in the upper atmosphere (typically at altitudes of 100-320 km), they transfer their energy, causing excitation of atmospheric particles4.
Atmospheric interactions: After colliding with atmospheric particles, the electrons lose most of their energy. Some may:
Continue interacting with other atmospheric particles
Be scattered in various directions, including back towards space
Gradually lose more energy and become part of the ionosphere4
Ionospheric dynamics: The ionosphere, where these interactions occur, is a dynamic region. While some electrons may escape back to space, others are continuously being produced through ionization processes2.
Electric fields and currents: The interaction between solar wind and Earth's magnetic field creates electric fields and currents in the ionosphere, which can influence the movement of charged particles2,3.
1. https://geo.libretexts.org/Bookshelves
2. https://www.nasa.gov/missions
3. https://www.swsc-journal.org/articles
4. https://mountwashington.org/the-science-of-auroras/
IONOSPHERE ELECTRIC CURRENT PROBLEMS
Electric currents in the ionosphere can indeed discharge to satellites and other objects in space. This phenomenon is part of a complex system of space weather effects that can impact technology both in orbit and on Earth's surface.
The interaction between solar wind and Earth's magnetic field creates electric fields and currents in the ionosphere, which can lead to several effects:
Satellite charging: Satellites can accumulate electrical charge from the ionospheric plasma, potentially leading to electrostatic discharges4. These discharges can cause phantom commands, damage to electronics, loss of control, and even satellite failure2.
Internal charging: Highly energetic electrons (>2 MeV) can penetrate satellite components, causing internal charging and possible electric discharges. This can result in malfunctions or complete failure of satellites2.
Magnetosphere-ionosphere "lightning": Large-scale energy transfers between the magnetosphere and ionosphere can occur, lasting for hours and transferring hundreds to thousands of times more energy than terrestrial lightning5. This process is enhanced during solar storms and can affect satellites and other space-based technologies.
GPS and communication disruptions: The ionospheric currents and associated plasma disturbances can interfere with radio signals passing through the ionosphere, potentially disrupting GPS navigation and satellite communications3.
Ground-based infrastructure impacts: Strong ionospheric currents can induce currents in long conductors on Earth's surface, such as power lines and pipelines, potentially causing power system outages or pipeline corrosion2.
These effects highlight the importance of understanding and predicting ionospheric dynamics to protect our technological infrastructure both in space and on the ground3,5.
1. https://www.swpc.noaa.gov/phenomena/ionosphere
2. https://www.spaceweather.gc.ca/tech/index-en.php
3. https://www.cnn.com/2024/08/02/science
4. https://www.nasa.gov/missions/icon
5. https://www.nasa.gov/solar-system
IONOSPHERE EFFECTS ON EM RADIATION
The ionosphere layers have significant effects on electromagnetic (EM) radiation, particularly in the high frequency (HF) range:
D Layer (50-90 km)
Primary effect: Absorption of radio waves
Absorbs lower frequency transmissions more strongly
Only present during daytime, disappears at night
E Layer (90-150 km)
Reflects radio waves with frequencies lower than about 10 MHz
Can reflect frequencies up to 50 MHz during intense sporadic E events
Weakens at night but still present
F Layer (150-500+ km)
Most important for long-distance HF radio communications
Splits into F1 and F2 layers during daytime
F2 layer (highest) has the greatest electron density
Main region for "reflection" (refraction) of HF radiation back to Earth
Remains active at night, allowing continued long-distance communications
General Effects
Reflection: Bends radio waves back toward Earth, enabling long-distance communication1,4
Refraction: Bends radio waves as they enter and exit the ionosphere3
Absorption: Particularly in the D layer, weakening signal strength1
Polarization: Rotates the polarization vector of radio waves3
For frequencies above 40 MHz, waves tend to penetrate through the ionosphere rather than being reflected3. The ionosphere's effects are most pronounced for frequencies below 40 MHz, with the E and F layers being the most important for reflection and long-distance propagation1,3.
IONOSPHERE CHANGES AT NIGHT
At night, the ionosphere undergoes several significant changes:
Thinning out: The ionosphere becomes less dense as previously ionized particles relax and recombine into neutral particles2.
Layer changes:
Reflection height: For very low frequency (VLF) waves, the reflection height changes from about 70 km during the day to about 85 km at night3.
Ionization source: Without solar radiation, cosmic rays become the primary source of ionization, though they are much weaker than the Sun's effect3.
Electron density: The F2 layer maintains a sizable density of electrons throughout the night due to downward diffusion of ions produced at high altitudes during the day4.
Radio propagation: Radio reception, particularly in the broadcast and shortwave bands, generally improves at night due to the disappearance of the D layer, which interferes with transmissions during the day4.
These nighttime changes in the ionosphere can lead to variations in radio signal propagation and potentially affect satellite-based communication and navigation systems.
MEGALIGHTNING DESTROYED COLUMBIA?
See https://www.columbiadisaster.info/
This shows Columbia’s vapor trail being struck by lightning in the ionosphere. The pic on the right is a closeup view of the one on the left.