Hugh Robin Farquhar Campbell What are the Northern Lights? The three conditions necessary for the aurora borealis to occur, solar winds of charged particles, the presence of a strong magnetic field, and a thick atmosphere, makes the northern lights a unique display among the rocky planets in our solar system. As a visible manifestation of solar activity, the Northern Lights signify great releases of energy from the sun, which cause great geomagnetic storms. As the root cause of the aurora borealis, the intensity of charged particles released by the sun is the determining factor in the strength of the Northern Lights visible at high latitudes. Due to the emission of extreme energy produced in the centre of the sun due to proton-proton fusion, the outer layer of the sun, the solar corona, reaches temperatures of nearly 1.1x106K, (Feldman, Landi, & Schwadron, 2005) at which temperatures, the highly ionised atoms and charged particles, such as protons and electrons, are travelling at average speeds of 145 km.s-1. While the escape velocity of the sun is 620km.s-1, due to the Maxwell-Boltzmann distribution of speeds, many particles have speeds greater than the escape velocity (Encrenaz, Bibring, & Blanc, 2003).The emission of plasma from the sun causes two types of solar wind, of which one is denominated the slow solar wind and travels at speeds of 400 km.s-1, and the other is named the fast solar wind, and travels at speeds of 750 km.s-1 (Marshall, 2010). Above active areas of the sun, usually sun spots, electrons and charged particles can be accelerated along the closed loops of magnetic fields called Helmet streamers, with the result that some of the charged plasma can become detached where the peak of the streamer is furthest from the sun (Kallenrode, 2004). If large amounts of plasma suddenly become detached, this results in a large emission of particles in the sun known as solar wind. Since the emission of slow solar wind depends on Helmet streamers, changing solar activity most affects emission of slow solar wind. By contrast, the less dense fast solar wind occurs due to coronal holes, where open, nonlooped, magnetic field lines cause plasma to be accelerated away from the sun, leaving the corona whence the plasma came cooler and less dense (NASA, 2013). The solar wind originating from coronal holes are faster due to acceleration along magnetic field lines. The fast solar winds are also affected by solar activity, and both the fast solar wind and slow solar wind peak every 11 year solar cycle, and the changing amounts of plasma hitting the earth’s atmosphere during the solar cycle dictates the strength of the aurora borealis. The earth’s magnetic field protects life on earth from bombardments of high energy solar plasma, and the magnetosphere present is what causes the Northern lights to appear where they do. The magnetic field caused by the electric currents produced due to movements of liquid iron in the earth’s mantle causes a giant magnetic field pattern to extend from the planet (What causes the Earth's magnetic field?). This magnetic field pattern is known as the magnetosphere, and the strength of the solar wind is such that the magnetosphere is squashed at the side pointing to the sun, while an elongated magnetotail is produced behind the earth. Incoming particles from the solar wind are most often deflected away from the earth by the magnetosphere, which thus protects life on earth from most charged solar wind particles, some of which have energies of 10 keV and could cause mutations in genetic structures, leading to cancers and mutated offspring (Rodríguez-Pacheco, 2014). However, there are some particles that have enough energy or the correct orientation to enter the magnetosphere. Charged particles entering from especially the magnetotail can be directed by and accelerated along the earth’s magnetic lines towards the direction of the North Pole, whence the magnetic field emanates, and the paths of most of these particles follow magnetic lines Hugh Robin Farquhar Campbell coming from latitudes of 80°, not 90°, as there are fewer magnetic field lines at 90° compared to 80. However, in a geomagnetic storm, caused by, for example, a coronal mass ejection, the magnetosphere is compressed and causes the magnetic field lines in the magnetosphere to become more concentrated, with the result that in geomagnetic storms solar particles being deflected more, so the Northern Lights can be seen in places of lower latitude (Balogh, 1999). Every eleven years, at the peak of solar activity, the solar winds are much stronger, and more plasma is released as solar wind, with the result that the Northern Lights are especially fantastic when solar activity is highest in the solar cycle, as the colliding charged particles with the air molecules causes the colours best associated with the Northern Lights. The colours of the Northern Lights are due to the way in which incoming charged particles collide with air molecules. Charged particles, comprising mainly electrons, due to lower mass hence higher speed with similar kinetic energies, are accelerated in the final few thousand kilometres as they align with the magnetic fields and are drawn in to the atmosphere (Reiff, et al., 1988). The result of this is that incoming electrons have very high energies, so collisions with molecules present in the air cause electronic transitions to occurs, which causes different frequencies of light to be emitted. Through triangulation of various aurorae, scientists have found that most aurorae occur at 80 km above the surface of the earth (Hansen). In one case, when ionised nitrogen - ionised when an incoming electron causes another electron to be removed - regains an electron, the energy released in forming the more stable nitrogen atom takes the form of a photon of a certain frequency, corresponding to a certain wavelength in according with the equation E=hf, where h is Plank’s constant. Nitrogen is more stable as an atom than an ion as the total spin, hence multiplicity, of the nitrogen atom is higher than in a nitrogen ion, resulting in greater stability, according to Hund’s Rule of Maximum Multiplicity (ChemWiki). Other transitions are caused by excited nitrogen or oxygen atoms returning to the ground state, with the energy drop released as a photon of frequency corresponding to the energy of the electronic transition. As a result of Quantum Mechanics, some electronic transitions are “forbidden” in Chemistry, and cannot occur. In particular, the Laporte electronic selection rule states that in an electronic transition parity should be inverted, from gerade to ungerade, and vice versa. Gerade in this case means that the orbital looks the same when reflected in the line of inversion, with the opposite being true for ungerade. The result of the Laporte selection rule is that a transition can occur between a p and an s orbital, which are ungerade and gerade severally, but a transition cannot occur between an s and an s orbital. However, there is a probability that if the atom is further raised to an excited state, the transition can occur (Lancashire, 2006). Since this transition is a function of probability, there is an average time until the electronic transition will happen from when the atom originally becomes excited. Very excited oxygen has its electronic transitions noticeable affected by the Laporte selection rule, as it takes approximate ¾ of a second to emit green light, and often 2 minutes to emit red light, since these transitions are forbidden. When the oxygen atom emits green light, the atom remains excited, which allows the further transition that causes red light. When excited atoms collide with unexcited molecules, some energy is transferred. This means that for oxygen the red light is seldom emitted, as many collisions with other molecules causes the oxygen atom to lose the excitation required to release red light (Atmospheric Optics). However, in the very upper reaches of the atmosphere, around 100 km above the ground, the air is nearly a vacuum and oxygen is atomised. Since oxygen atoms here collide very seldom with other atoms, the oxygen atoms remain excited long enough to emit the red light. Hugh Robin Farquhar Campbell During the peak of a solar cycle, when there are very many sunspots, Helmet streamers allow large amounts of solar plasma to detach from the sun and travel as the solar wind. The charged particles are mostly deflected by the magnetosphere surrounding the earth; however, some particles manage to pass through and into the magnetosphere, and are accelerated along the magnetic field lines towards the high latitudes. During a geomagnetic storm, continual bombardment of the magnetosphere causes distortion of the magnetic field, and more particles are able to enter the magnetosphere and hit the atmosphere at lower latitudes. The incoming charged particles excite the oxygen and nitrogen molecules in the air, and cause the nitrogen, at lower altitudes, to emit green and blue light when electronic transitions occur or an electron is gained, respectively. However, Quantum Mechanical selection rules mean that some electronic transitions take much longer to occur, and in oxygen atoms, these forbidden mechanisms can only occur at high altitudes, where collisions are rare, leaving time to produce the red and green light. Bibliography Atmospheric Optics. (n.d.). Glowing Gases - Aurorae. Retrieved 25 02, 2015, from atoptics: http://www.atoptics.co.uk/highsky/auror3.htm Balogh, A. G. (1999). Corotating Interaction Regions. Springer. ChemWiki. (n.d.). Hund's Rule. Retrieved 2 25, 2015, from ChemWiki: http://chemwiki.ucdavis.edu/Inorganic_Chemistry/Electronic_Configurations/Hund%27s_Ru les Encrenaz, T., Bibring, J.-P., & Blanc, M. (2003). The Solar System. Springer. Feldman, U., Landi, E., & Schwadron. (2005). On the Sources of Fast and Slow Solar Wind. Journal of Geophysical Research, 110. Hansen, T. L. (n.d.). The Northern Lights - What are they? Retrieved 2 25, 2015, from geophysics: http://geo.phys.uit.no/articl/theaurora.html Kallenrode, M.-B. (2004). Space Physics: An Introduction to Plasmas and Particles in the Heliophere and Magnetopheres. Berlin: Springer. Lancashire, R. J. (2006). Selection Rules for Electronic Spectra of Transition Metal Complexes. In R. J. Lancashire, Selection Rules for Electronic Spectra of Transition Metal Complexes. Mona: University of the West Indies. Marshall, N. (2010). GCSE Astronomy. Mickledore . NASA. (2013, 6 18). Massive Coronal Hole on Sun. Retrieved 2 24, 2015, from NASA.gov: http://www.nasa.gov/mission_pages/sunearth/news/gallery/20130618coronalhole.html#.VOyRc3ysWVN Hugh Robin Farquhar Campbell Reiff, P. H., H L, C., J D, C., J L, B., J D, W., E G, S., et al. (1988). Determination of auroral electrostatic potentials using high and low-altitude particle distribution. Journal of Geophysical Research, 93. Rodríguez-Pacheco, J. (2014, 9 1). Solar Energetic Particles. Retrieved 2 24, 2015, from cifs-isss.org: http://www.cifs-isss.org/presentazioni/2014-september/Pacheco.pdf What causes the Earth's magnetic field? (n.d.). Retrieved 2 25, 2015, from Physics.org: http://www.physics.org/article-questions.asp?id=64
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