By Malcolm P.R. Light
August 10, 2012 
Abstract 
The exponential increase in the Arctic atmospheric methane derived from the destabilization of the subsea Arctic methane hydrates is defined by both the exponential decrease in the volume of Arctic sea ice due to global warming and the exponential decrease in the continent wide reflectivity (albedo) of the Greenland ice cap caused by increasing rates of surface melting which reach minima around 2014, 2015. 
The high anomalous atmospheric methane contents recorded this year at Barrow Point Alaska (up to 2500 ppb - Carana 2012b) and the fact that the surface atmospheric methane contents may be linked via a stable partial pressure gradient with increased maximum methane contents in the world encompassing global warming veil (estimated at ca 1460 ppb methane) makes it imperative that the Merlin lidar satellite be launched as soon as is feasibly possible. The Merlin lidar satellite will give us a clear idea of how high the Earth’s stratospheric methane concentrations are in this poorly documented giant methane reservoir formed above the ozone layer at 30 km to 50 km altitude (Ehret, 2010). 
Methane detecting Lidar instruments could also be installed immediately on the International Space Station to give early warning of the methane buildup in the stratosphere and act as a back up in case the Merlin satellite fails. 
Unless immediate and concerted action is taken by governments and oil companies to depressurize the Arctic subsea methane reserves by extracting the methane, liquefying it and selling it as a green house gas energy source, rising sea levels will breach the Thames Barrier by 2029 flooding London. The base of the Washington Monument (D.C.) will be inundated by 2031. Total global deglaciation will finally cause the sea level to rise up the lower 35% of the Washington Monument by 2051 (68.3 m or 224 feet above present sea level). 
Introduction
Recent atmospheric methane observations (May 01, 2012) at Barrow Point Alaska  show extreme methane concentrations as high as 2500 ppb (2.5 ppm Methane,  Figure 1)(Generated by ESRL/GMD May 01, 2012 from Carana, 2012b). The  present atmospheric methane concentration at Point Barrow exceeds all previous  measurements in the Arctic and if it represented the mean atmospheric concentration after an extended period of subsea Arctic methane emission (10 to 20 years) at a  methane global warming potential (GWP) of 100 (Dessus et al. 2008) it would be  equal to a 2.5 degrees C mean global temperature increase and a methane-carbon output of  some 6 Gt. This would be equivalent to adding and extra 250 ppm of carbon dioxide  to the atmosphere or about 2/3 of the present carbon dioxide content.
The rising light Arctic methane migration routes have been interpreted on the Hippo  profile in Figure 2a (from Wofsy et al. et al. 2009) using the inflexion points on the  temperature and methane concentration profiles similar to the system used to identify  deep oceanic current trends using salinity and temperature data (Tharp and Frankel,  1986). The light Arctic methane is rising almost vertically up to the stratosphere  between 60o North and the North Pole. This is consistent with the methane rising in  the same way as hydrogen with respect to the cold dry polar air because it has almost  half the density of air at STP(Engineering Toolbox, 2011) (methane in wet air may be  transported horizontally by storm systems). In addition because methane has a global  warming potential of close to 100 during the first 15 to 20 years of its life (Dessus et  al. 2001) it will preferentially warm up and expand compared to the other atmospheric  gases and thus drop even further in density making it much lighter than the air. This  methane rises into the upper stratosphere where it is trapped below the hydrogen  against which it has an upper diffuse boundary as shown by the fall off in methane  concentration between 40 km and 50 km altitude (Figure 2a after Nassar et al. 2005).
It is clear from the flattening of the methane concentration trend in the stratosphere  between 30 km and 47 km (Nassar et al. 2005) that this probably represents an  expanding, world encompassing methane global warming veil (Figure 2a after  Nassar et al. 2005). This stratospheric methane is above the ozone layer and it appears  entirely stable between 30 km and 40 km where it shows little change (Figure 2a  after Nassar et al. 2005). It is therefore very likely that the methane global warming  veil will form a giant reservoir for quickly rising low density methane emitted into  the dry Arctic atmosphere by progressive destabilization of subsea Arctic methane  hydrates (Light, 2011, 2012) combined with smaller amounts of methane formed  by methanogenesis (Allen and Allen, 1990; Lopatin 1971). Much of the dry, light  methane is able to bypass the ozone layer unimpeded in a tropospheric - stratospheric  circulation system to be discussed later.
There is a transition zone from about 60o to 65o North where the methane begins to spiral outwards from the Arctic region towards the mid latitudes and upwards towards the stratosphere to reach the base of the ozone layer where it is being mixed into the  stratosphere by giant vortices active at different times (Light 2012; NSIDC 2011a).
The continuous vertical motion of the methane in the Arctic region as it rises to the  stratosphere between 60o to 65o North which has a lateral motion impressed on it at lower latitudes must set up a methane partial pressure - concentration gradient between the Arctic surface atmospheric methane emissions and the stratospheric methane global warming veil. Therefore any marked increase in the surface methane concentration and partial pressure should be marked by similar increases in the upper  stratosphere within the methane global warming veil.
A further consequence of the light methane rising like hydrogen into the upper  stratosphere where it forms a stable zone beneath the hydrogen between 30 km and  50 km height, is that this methane is never recorded in the mean global warming gas  measurements made at Mauna Loa. We therefore have a completely separate high  reservoir for methane, which at the moment we only have vague information on  and it may contain sufficient methane gas to multiply the Mauna Loa readings by a  considerable amount.
Graphic Display of The Effects of the Methane Warming Veil
Figure 2b is a graphic display of the atmosphere from 0 to 55 km altitude versus  increasing Arctic atmospheric methane concentration reaching up to 6000 ppb (6  ppmv methane). The troposphere, tropopause, stratosphere, stratopause, mesosphere,  and ozone layer are from Heicklen, 1976. The various events related to global  warming (droughts, water stress, coral bleaching and death, deglaciation, sea level  rise and major global extinction) are from Parry et al. 2007.
Figure 2b has been designed to graphically portray the growth of the subsea Arctic  atmospheric methane as new observations become available and how this build up  strengthens the methane concentration in the stratosphere where it forms a world  encompassing methane global warming veil at an altitude of 30 km to 47 km.  Figure 2b will be used to progressively chart mankind's Arctic methane emission,  exponential expressway to extinction within the next half century.
As the light-rising Arctic methane is spread around the world by the Arctic  stratospheric vortex system (NSIDC 2011a), it can be expected to lead to more ozone  and water vapor in the stratosphere, both of which will add to the greenhouse effect  and thus cause temperatures to increase globally. In the Arctic, where there is very  little water vapour in the atmosphere, the ozone layer may well be further depleted,  because the rising methane behaves like a chloro-fluoro-hydrocarbon (CFC) under  the action of sunlight increasing the damaging effects of ultraviolet radiation on the  Earth’s surface (Engineering Toolbox, 2011; Anitei, 2007). Large abrupt releases of  methane in the Arctic lead to high local concentrations of methane in the atmosphere  and hydroxyl depletion, making that methane will persist longer at its highest  warming potential, i.e. of over 100 times that of carbon dioxide. (Carana, 2011a).  The presence of a large hole in the Arctic ozone layer in 2011 is most likely a result  of this same process of ozone depletion caused by a buildup of greenhouse gases from  the massive upward transfer of methane from the Arctic emission zones through the  lower stratosphere up into the stratospheric veil between 30 km and 47 km height  (Science Daily, 2011).
Anomalous Arctic Atmospheric Methane Concentrations
The extremely high content of atmospheric methane measured in May 2012 at Barrow  Point Alaska (2500 ppb) represents a very dangerous turn of events in the Arctic and  further substantiates the claim that the whole Arctic has now become a latent subsea  methane hydrate sourced blowout zone which will require immediate remedial action  if there is any faint hope of containing the now fast increasing (exponential!) rates of  methane eruptions into the atmosphere (Light 2012c - Angels proposal; see end of this  text).
The exponential increase in the Arctic atmospheric methane content from the  destabilization of the subsea methane hydrates is defined by the exponential decrease  in the volume of Arctic sea ice caused by the resulting global warming due to the  build up of the atmospheric methane (Carana, 2012d).  The exponential increase in the Arctic atmospheric methane is also implied by an  exponential decrease in the continent wide reflectivity (albedo) of the Greenland ice  cap caused by increasing rates of surface melting (Figure 3; NASA Mod 10A1 data,  from Carana, 2012c).
Albedo data for Greenland shows that it will become free of a continuous snow cover  by about 2014, so that the underlying old ice cover which has low reflectivity will  be totally exposed to the sun in the summer (Carana, 2012c). This darker material will  become a major heat absorber after 2014 starting the fast melt down of the Greenland  ice cap and this process will probably affect the older ice in the floating Arctic sea ice  fields. The Arctic ocean will also become free of sea ice by 2015 exposing the low  reflectivity ocean water directly to the sun, causing a high rate of temperature rise in  Arctic waters and the consequent destabilization of shelf and slope methane hydrates  releasing large volumes of methane into the atmosphere (Carana, 2012d; AIRS data Yurganov, 2012).
As a consequence, the enhanced global warming will melt the global ice sheets at a  fast increasing rate causing the sea level to begin rising at 15.182 cm/yr in the first  few years after 2015 giving an accurate way of gauging the worldwide continental  ice loss (Figure 3). This sudden increase in the rate of sea level rise will mark the last  moment mankind will have to take control of the Arctic wide blowout of methane into  the atmosphere and a massive effort must be made by governments and oil companies  to stem the flow of the erupting subsea methane in the Arctic before this time. The  loss of complete snow cover in Greenland precedes the loss of the sea ice cap in  the Arctic by a year which may be due to the more extreme weather conditions that  usually prevail over continents than over the sea which moderates the weather.
Methane and Ozone Circulation
The components of the atmosphere undergo diffusion by a number of processes. The  mean speed of horizontal displacement of the stratosphere around the Earth is known  to be about 120 km/hr from the Krakatoa eruption in 1883 (Heicklen, 1976). Winds  also transfer material northward and southward in the stratosphere in quite a different  pattern to that of the tropospheric wind flows (Heicklen, 1976). Mean wind velocities  within the global methane warming veil and above it (36 km to 91 km altitude) are  some 48 m/sec during the day and 56 m/sec at night (Olivier 1942, 1948). Large  latitudinal variations in the atmospheric density at 100 km altitude require meridional  flows of 10 to 50 m/sec (Heicklen, 1976).
At subarctic latitudes at the height of the global methane warming veil (30 km to 50  km altitude) the ozone concentration lies between 1.7 to 1.9*10^12 molecules/cc to  5.4*10^10 molecules/cc and does not vary during the day (Heicklen, 1976). The sub-arctic ozone reaches a maximum in the lower stratosphere in winter at an altitude of  17 km to 19 km (7.7*10^12 molecules/cc) and in summer at an altitude of 18 km to  19 km (5.1*10^12 molecules/cc)(Heicklen, 1976).
The seasonal variation of ozone in the stratosphere in Arctic latitudes is caused  by a circulation transfer system which moves ozone from the upper stratosphere  in equatorial and mid-latitudes to the Arctic lower stratosphere during the winter  (Heicklen, 1976). The stored Arctic lower stratospheric ozone is lost in the summer  by chemical dissociation when it moves downwards or by photosynthetic destruction  if it moves upwards (Heicklen, 1976).
The Hippo methane concentration and temperature profiles shown in Figures 2a  and 2b extend from the surface to some 14.4 km altitude and from the North Pole  southwards across the Equator to a latitude of -40o south (Wofsy et al. 2009). As  already described the methane flow trends on Hippo methane concentration and  temperature profiles have been interpreted in detail using a similar system to that used  by the Meteor expedition in determining deep ocean circulation patterns from salinity  and temperature data (Figure 2a - see Tharp and Frankel, 1986).
Methane erupted from destabilizing methane hydrates in the subsea Arctic and of  methanogenic origin has almost half the density of air at STP in dry Arctic conditions  and is seen to be rising vertically to the top of the Troposphere between 70o North and  the North Pole on the Hippo methane concentration profiles (Engineering Toolbox,  2011; Wofsy et al. 2009 ). On the Hippo data, at latitudes less than 70o North, the  rising methane clouds are being spun out and laterally spread in the middle and upper  troposphere and upper stratosphere by stratospheric vortices (NSIDC, 2011a). The  methane appears to be entering the lower stratosphere in the low latitudes between  25o North and the equator which it then overlaps and is carried into the Southern  Hemisphere to almost -40o South (Figure 2a)(Light 2011c). In the equatorial regions  the growth of the methane global warming veil will amplify the effects of El Nino in  the Pacific further enhancing its deleterious effects on the climate.
As this vertically and laterally migrating methane enters the stratosphere in equatorial  and mid-latitude positions it is helping to displace the equatorial and mid-latitude  ozone which migrates downwards and northwards towards the north pole (Heicklen,  1976) to complete the cycle. The methane may be partly drawn up into the lower  and upper stratosphere by a global pressure differential set up by the poleward and  downward motion of the ozone (Heicklen, 1976) Once the methane has entered the  stratosphere and has helped to displace some of the ozone, it is able to accumulate  in the upper stratosphere beneath the hydrogen as a continuous stable layer between  30 and 47 km forming a world wide global warming veil (Figures 2a and 2b; Light  2011c).
In the Arctic region methane has been shown to rise nearly vertically and is locally  charging the global warming veil in addition to methane that has diffused from mid  latitude and equatorial regions. There must therefore exist a partial pressure gradient  between the Arctic surface methane anomalies and the upper stratosphere methane  global warming veil such that any increase of the surface methane concentration and  partial pressure should lead to a transfer of methane into the upper stratosphere and  to a similar increase in the partial pressure and concentration of the methane there.  The methane partial pressure gradient that exists between the anomalous Arctic ocean  surface methane emissions and the stratospheric methane global warming veil at 30  km to 47 km height is partly controlled by the complex motions and reactions of the  Arctic ozone layer which separates the troposphere from the upper stratosphere and  shows little variation in the day or between summer and winter (Heicklen, 1976).
Consequently the concentration of the methane in the upper stratospheric global  warming veil should track the increase of Arctic atmospheric methane to some  degree and knowledge of the latter can allow absolute maximum estimates to be  made on the magnitude of the former. This will give a rough estimate of what the  highest value the methane concentration is likely to reach within the global warming  veil within the Arctic area. This is a worst case scenario which has to be assumed in  order to prevent Murphy’s law being operative (i.e. if anything can go wrong, it will  go wrong in estimating the maximum methane value). An alternative is to view this  solution of the methane concentration in the global warming veil as German over-engineering in order to eliminate any possible errors in the estimate of the maximum  value. My Father, a Saxon would have commended me on this approach. This is  precisely what mainstream world climatologists have failed to do in their modeling  of the effects of Arctic methane hydrate emissions on the mean heat balance of the  atmosphere and why we are now facing such a severe climatic catastrophe from  which we may very likely not escape. Let us hope and pray that the Merlin Lidar  methane detection satellite does not find methane magnitudes in the Arctic global  warming methane veil (30 km – 47 km altitude) at the levels predicted in this paper,  when it is launched in 2014.
The maximum global methane veil concentration in the mid latitudes (30o to 60o North) between 30 km and 40 km altitude was estimated by occultation at some 0.97 ppmv methane (970 ppb) between February to April, 2004 (Nassar et al. 2005). In  2004 - 2005 the Arctic atmosphere at Point Barrow, Alaska reached an anomalous  maximum of some 2.014 ppmv methane (2014 ppb)(Carana, 2012e). This means that  the most extreme methane concentration anomalies in the Arctic (Point Barrow) are  leading the maximum concentration in the global warming methane veil by some  1.044 ppmv methane (1044 ppb). Consequently as a first rule of thumb assuming that  the vertical methane partial pressure gradient has remained relatively unchanged, we  can estimate the maximum methane concentration within the Arctic methane global  warming veil between 30 km and 47 km height by subtracting 1.044 ppmv methane  (1044 ppb) from measured surface Arctic atmospheric value at the same time.
High methane concentrations of 2 ppmv (2000 ppb) were being reached in the Arctic  in 2011 (position a. in Figure 2b) similar to those recorded in 2004 – 2005 at Point  Barrow Alaska (Carana, 2012e). It is therefore likely that by 2011 that the maximum  concentration of methane in the methane global warming veil had remained relatively  unchanged since 2004. This is consistent with the start of major methane emissions in  the Arctic in August 2010 as recorded at the Svalbard station and in the East Siberian  Shelf in 2011 which would not have given the emitted gases sufficient time to reach  the upper stratosphere(Light, 2012a, Shakova et al. 2010a, b and c).
On May 01, 2012 an atmospheric methane concentration of 2.5 ppmv (2500 ppb)  was recorded at Point Barrow indicating an increase in the maximum methane  concentration anomaly of 0.5 ppmv methane (500 ppb) in one year (yellow spike  on Figure 1; position b. in Figure 2b)(ESRL/GMO graph from Carana 2012b). We  can therefore predict conservatively that the maximum concentration of the methane  in the Arctic stratospheric methane global warming veil between 30 km and 47 km  altitude may be as high as 1.456 ppmv methane (1456 ppb) (= 2500 -1044 ppmv)  (position b. in Figure 2b)(ESRL/GMO graph from Carana 2012b).
Assuming that the maximum Arctic surface atmospheric methane content continues  to increase now at a rate of 0.5 ppmv (500 ppb) each year we can roughly predict  that by 2013 it will have reached 3 ppmv (3000 ppb) and by 2014, 3.5 ppmv (3500  ppb) which is when the Merlin Lidar methane detection satellite will be launched  (Ehret, 2010). Using the previous method of predicting the maximum likely methane  content in the Arctic methane global warming veil between 30 km and 47 km altitude,  the maximum for 2013 is 1.956 ppmv methane (1956 ppb)(position c. in Figure 2b)  and for 2014 is 2.456 ppmv methane (2456 ppb) (position d. in Figure 2b). This  means that by the time the Merlin Lidar satellite is launched the Arctic Ocean will  have emited sufficient methane to have surpassed the 2oC anomaly limit. Once the  entire atmospheric mean exceeds a 2oC temperature increase it will precipitate fast  deglaciation, the start of widespread inundation of worldwide coastlines, extensive  droughts and water stress for billions of people (Figure 2b)(after Parry et al. 2007).
This high predicted concentration of methane in the Arctic methane global warming  veil in 2014 is consistent with the exponentially falling albedo data for the Greenland  ice cap which suggests that major melting will begin in 2014 (Carana, 2012c). The  exponential reduction in volume of the Arctic sea ice to zero in 2015 (Carana, 2012d) will precipitate a massive increase in the release of Arctic  subsea methane from destabilization of the methane hydrates as the dark ice free  Arctic ocean absorbs large quantities of heat from the sun (Light, 2012a).
MERLIN Lidar Satellite
The MERLIN lidar satellite (Methane Remote Sensing Lidar Mission) , which is  a joint collaboration between France and Germany will orbit the Earth at 650 km  altitude and will be able to detect the methane concentration in the atmosphere  from 50 km altitude to the surface of the Earth (Ehret, 2010). The Lidar methane  detection instrument was jointly developed by DLR (Deutches Zentrum für Luft –und  Raumfahrt), ADLARES GmBH and E. ON Ruhrgas AG (Ehret, 2010).
This satellite is scheduled to be launched sometime in 2014 (Ehret, 2010) and will be  the first time that real time data will be able to detect the concentration of methane  within the world encompassing methane global warming veil between 30 km and  47 km altitude and give us the first detailed picture of the size of the beast we are  dealing with. Previous indications of this layer in the mid latitudes was made using occultation (Nassar et al. 2005)
The high anomalous atmospheric methane contents recorded this year (May 01)  at Barrow Point Alaska (see Figure 2b, Carana 2012b) and the fact that they may  be linked via a stable partial pressure gradient with increased maximum methane  contents in the world encompassing global warming veil (estimated at ca 1456 ppb  methane) makes it imperative that the Merlin lidar satellite be launched as soon as  is feasibly possible so we can get a clear idea of how high the Earth’s stratospheric  methane concentrations are. The Merlin satellite will continuously give us real time  information on the size of the stratospheric methane global warming veil that is  gathering its strength in the upper atmosphere.
This information shows how extremely serious the Arctic methane emission problem  is and how urgently we need to measure the status of the Arctic stratospheric methane  global warming veil between 30 km and 47 km height. An early warning of high  methane contents in the methane global warming veil will give humanity time to react  to the existing and new threats that are developing in the Arctic.
Methane detecting Lidar instruments could also be installed immediately on the  International Space Station to give us early warning of the methane build up in the  stratosphere and act as a back up in case the Merlin satellite fails.
Sea Level Rise
The progressive rise in sea level from 2015 is shown on Figures 3, 4 and 5. Figures  4 and 5 are simplified versions of Figures 7, 8 and 9 in Light 2012a and Figures  12 and 13 in Light 2012c. The various events related to global warming (droughts,  water stress, coral bleaching and death, deglaciation, sea level rise and major global  extinction) are from Parry et al. 2007. At the time of total worldwide deglaciation, the  sea level is estimated to rise some 68.3 metres (224 feet) (Wales, 2012)
The maximum time of inundation of various coastal cities, coastlines and coastal  barriers is shown on Table 1 (after Hillen et al. 2010; Hargraves, 2012). Rising sea  levels will breach the Thames Barrier by 2029 flooding London. The base of the  Washington Monument (D.C.) will be inundated by 2031. Total global deglaciation > will cause the sea level to rise up the lower 35% of the Washington Monument by  2051 (68.3 m or 224 feet above present sea level).
Because of the massive increase in the strength of the storm systems and waves, high  rise buildings in many of the coastal city centers will suffer irreparable damage and  collapse so that the core zones of the cities will be represented by a massive pile of  wave pulverised debris. Unfortunately by that time a large portion of sea life will be  extinct and the city debris fields will not form a haven for coral reefs. The seas will  probably still be occupied by the long lasting giant jellyfish (such as are now fished  off Japan), rays and sharks (living respectively since 670, 415 and 380 million years  ago) and the sea floor by coeolocanths (living since 400 million years ago)(Calder,  1984). The city rubble zones will probably be occupied by predatory fish (living since  425 million years ago)(Calder 1984). Life will also continue in the vicinity of oceanic  black smokers so long as the oceans remain below boiling point.
ANGELS Proposal
If left alone the subsea Arctic methane hydrates will explosively destabilize on their  own due to global warming and produce a massive Arctic wide methane “blowout”  that will lead to humanity’s total extinction, probably before the middle of this  century (Light 2012 a, b and c). AIRS atmospheric methane concentration data  between 2008 and 2012 (Yurganov 2012) show that the Arctic has already entered the  early stages of a subsea methane “blowout” so we need to step in as soon as we can  (e.g. 2015) to prevent it escalating any further (Light 2012c).
The Arctic Natural Gas Extraction, Liquefaction & Sales (ANGELS) Proposal aims  to reduce the threat of large, abrupt releases of methane in the Arctic, by extracting  methane from Arctic methane hydrates prone to destabilization (Light, 2012c).
After the Arctic sea ice has gone (probably around 2015) we propose that a large  consortium of oil and gas companies/governments set up drilling platforms near the  regions of maximum subsea methane emissions and drill a whole series of shallow  directional production drill holes into the subsea subpermafrost “free methane”  reservoir in order to depressurize it in a controlled manner (Light 2012c). This  methane will be produced to the surface, liquefied, stored and transported on LNG  tankers as a “green energy” source to all nations, totally replacing oil and coal as the  major energy source (Light 2012c). The subsea methane reserves are so large that  they can supply the entire earth’s energy needs for several hundreds of years (Light  2012c). By sufficiently depressurizing the Arctic subsea subpermafrost methane  it will be possible to draw down Arctic ocean water through the old eruption sites  and fracture systems and destabilize the methane hydrates in a controlled way thus  shutting down the entire Arctic subsea methane blowout (Light 2012c).
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Minggu, 12 Agustus 2012
Charting Mankind’s Arctic Methane Emission Exponential Expressway to Total Extinction in the Next 50 Years
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