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					 HELIUM and INERT GAS BASICS The inert, or 
					noble, gases comprise 
					helium, neon, argon, krypton, xenon, and radon, 
					of which helium is probably the most important. 
					They 
					are formed during the natural 
					radioactive decay of elements such as uranium and thorium 
					within the interior of the Earth.
 
 Helium is a valuable inert gas used in
					commercial, military, and medical applications. It doesn't
					burn or combine chemically with other elements.
 
 It has
					unusual cryogenic properties and is used in welding to cool
					material adjacent to the weld and to cool the magnets in MRI 
					machines, as well as the magnets at CERN that helped 
					discover the Higgs boson. It also fills kids' balloons, 
					weather balloons, dirigibles,  makes your voice
					go squeaky when you breathe it, and helps space ships get
					off the ground.
 
 Helium and other 
					inert gases are often found
					in conjunction with carbon dioxide and nitrogen, in wells that were originally drilled for
					oil or natural gas as early as 1903 (in Kansas). This
					discovery led to development, by the US government,  of
					a large helium resource stretching from Kansas through
					Oklahoma into the panhandle of Texas. Pipelines, separation
					facilities, and a large strategic reserve storage facility
					were built during the 1950's and 1960's. Some processing was
					privatized in the 1960's and private development was
					permitted from the 1990's. Canada and Poland produced small
					quantities in the 1960's and 1970's.
 
 
 
  
 
 
 
 
 
 
 
 
 
 
 
 
 <==
					Map of US helium reservoirs in mid-continent region. Image
					courtesy US BLM.
 
 
 
 
 
 
 
 Today, the USA produces about 55% of World supply, Algeria
					and Qatar about 40%, the balance from a half dozen other
					countries. The price is a little volatile, averaging US$
					100+/- per thousand cubic feet (mcf), compared to natural
					gas at US$ 4.00+/-.
 
 Gas analysis reports
					from helium bearing wells show high concentrations of CO2
					or N2 with traces to several percent helium. Some have
					hydrocarbon gases (methane, ethane, propane) in quantities
					too small to allow the gas mixture to burn. A typical
					analysis might show 5% He and 95% N2, or 5% He with 95% CO2,
					or 5% He, 35% methane, with 60% N2. Wells with less than
					0.5% He are probably uneconomic; an average producing well
					in the USA has about 4% He.
 
 
				
					
						
						The method used to separate helium 
						from a gas mixture is fractional distillation to 
						create crude helium, followed by low temperature liquefaction 
						to produce Grade-A 99.995% pure helium. 
					The major source of helium is
					radioactive decay of uranium and thorium in basement rocks
					or shales below potential reservoirs. Many helium producing
					fields are associated with volcanic intrusions or deep-seated basement shears. Some helium may also come from
					the primordial lithosphere through faults; this is the
					lighter isotope of helium. Few isotope ratios have ever been
					performed so the source is not precisely known in many
					cases.
 
 
					To trap helium in a reservoir
					you need the same geological setting as for natural gas:
					source rock, migration path, porous reservoir rock,
					structural or stratigraphic trap, and a seal at the top of
					the trap. 
					  
					Migration path is usually
					through faults or fractures but could be direct contact of a
					reservoir with a source rock. Reservoirs are  usually
					sedimentary strata, but some igneous rocks may be porous and
					permeable enough to hold helium. 
					  
					Traps are often structural,
					as drape over domes or anticlines. Strat traps are harder to
					seal. The seal is more critical than for conventional oil or
					gas. The helium molecule is about half the size of a methane
					molecule so it can penetrate through smaller pores and
					fractures than methane. This makes it difficult to contain
					in samples and the seal on any trap must be lower
					permeability than a similar trap for oil or natural gas. The
					best seals are salt, salt plugged porosity, lava flows, or
					very fine claystone (shale).
 Production rates vary with reservoir quality, thickness, and
					pressure. Many were overpressured and blew out in the early
					days of helium exploration. CAUTION: If you find production
					rates or production rate graphs, be sure to distinguish
					between total flow rate of all gases versus helium flow
					rates -- it isn't always clear.
 
 If you are concerned about the environment, the inert gases,
					other than helium, are vented to the atmosphere, including
					CO2
					and any hydrocarbons in the mixture. A few wells are
					actually completed to capture CO2 or N2 for commercial
					purposes, but most are not.
 
 
					
					 Distribution of all known helium tests in the lower
					Paleozoic: Deadwood, Winnipeg, Red River and Stony Mountain
					formations. Image from "Helium in Southwestern Saskatchewan", Melinda
					Yurkowski, Saskatchewan Geological Survey, Open File Report
					2016-1
 
					
					
  LOG ANALYSIS IN HELIUM WELLS Petrophysical analysis of inert gas reservoirs involves the
					same steps as any other gas well: shale volume, effective
					porosity, lithology, water saturation, permeability,
					gas-in-place. There are a number of pitfalls in analyzing the well logs in
					helium bearing zone in addition to the usual problems of
					rough hole condition, highly variable mineralogy, salt
					plugged porosity, and varying water resistivity which can
					occur in any well. Here are the critical things that need to
					be considered:
 
 1. Old wells have minimum log suites (Electrical survey (ES),
					possibly a microlog (MLC). By 1960 there may be a single
					transmitter sonic log, by 1965 possibly a density log, and if
					the God's are willing, a gamma ray and neutron log (GRN), probably
					through casing. Each of these logs require special handling,
					covered elsewhere in this Handbook, BUT ALSO subject to all
					the concerns listed below.
 
 2. All porosity models must be corrected for shale volume.
					The gamma ray may permit this, but it should be calibrated
					to XRD clay volume on at least a few samples.
 
 3. Inert gases have no hydrogen, so in theory the neutron log reads zero
					porosity. In air-drilled holes, there is no 
					mud-filtrate invasion, so neutron reads near zero. On 
					liquid-filled holes, neutron varies somewhat with the actual
					water saturation in the invaded zone and depth of investigation 
					of the log. Clay volume, and
					whether or not the gas column contains hydrocarbon gas in
					addition to
 
					the inert gases will increase neutron porosity  In some wells, invasion is
					deep enough for the neutron log to read a reasonable
					porosity value. In other wells, the neutron log reads zero
					or even slightly negative apparent porosity.
 4. Sonic and density logs when transformed to porosity will read too high
					a porosity due to gas effect, unless invasion is very deep
					and residual gas in the invaded zone is negligible
					(unlikely). Standard gas correction models will be needed,
					calibrated to core porosity. Variations in matrix rock properties
					will need to be controlled by sample and core description.
 
 5. With the neutron log reading too low compared to a hydrocarbon gas
					(possibly near zero),  the standard gas corrected
					density neutron complex lithology model for porosity may not
					work well, giving a porosity that is too low. Some limited
					experience in Saskatchewan suggests that invasion may be
					sufficient to minimize this problem, but there was no core
					data available to prove this. In other project areas, the
					neutron reads zero and cannot be used as a porosity
					indicator.
 
 6. NMR porosity is unaffected by clay, mineralogy, or gas effects, so it
					will give a reliable porosity in inert gas reservoir,
					provided the borehole is not too rough and there is some
					drilling fluid invasion. Some core analysis
					control is comforting but less essential than for sonic and
					density porosity.
 
 7. The only lithology model that works properly in a gas reservoir is the
					PE 2-mineral model. The PE curve was not common until the
					1990's and may be missing in many wells drilled after that
					date, so there may be no direct method to calculate
					mineralogy. Sample and core descriptions are a necessity to assist
					in understanding the mineralogy and the higher quality
					reservoir faces.
 
 8. After a porosity algorithm has been calibrated to core, the deep
					resistivity can be used to calculate water saturation,
					provided the correct RW regime can be identified. This
					allows the calculation of total gas in place. Multiply by
					helium fraction to obtain helium in place.
 
 9. If salt plugging is present, it might be possible to identify it by
					very high resistivity and very low neutron and/or NMR porosity. The
					efficacy will depend on whether or not the drilling fluid
					has dissolved the salt in the zone investigated by the
					neutron log. Sonic and density porosity may be lower than
					non-plugged intervals due to the different log response of
					salt and gas. Results may still be ambiguous. When identified, salt plugged zones are flagged and porosity set
					to zero.
 
 10. Once porosity and saturation are calculated, and salt plugged
					intervals are flagged, permeability can be calculated from
					the usual Wyllie, Timur, or Lucia methods. An estimate of
					total gas deliverability at initial unstimulated conditions
					is possible based on the sum of permeability thickness
					values. There is a large possible error in this result as
					natural fracture permeability is not included.
 
					  
					  11. Helium concentration
					CANNOT be calculated directly from any well log result.
 12.
					Inert gas wells are among the most difficult to quantify
					using well log data. Core analysis data and sample
					descriptions, with a little help from XRD mineralogy data,
					can make the job a little more
 conclusive. Commercial software will most likely fail to give an accurate 
					estimate of porosity unless you add some user-defined 
					equations to account for the peculiar gas  effect 
					caused by inert gases..
 
 
  LOGging program for inert gas wells While we are stuck with the log suite in existing wells, we
					can run an appropriate program today that will give optimum
					results. The recommended suite is:
 
 1. array induction or array laterolog with SP and gamma ray. (In 
					air-drilled holes, laterolog cannot be run).
 2. density neutron with PE and spectral gamma ray.
 3. nuclear magnetic resonance log with gamma ray.
 4. array sonic log for correlation with older wells and to assist seismic
					interpretation.
 5. resistivity image log to assist in facies description, and trap
					and seal definition.
 
 Items 3 and 5 are needed only from TD to 100 meters above
					the zone of interest.
 
 Gas log, conventional or drilled sidewall cores, close
					spaced sample description, and XRD mineralogy and bulk clay
					are strongly recommended.
 
 
 
  LOG ANALYSIS EXAMPLES IN HELIUM WELLS 
 
  ANCIENT LOG EXAMPLES WITH NO QUANTITATIVE PETROPHYSICAL
					ANALYSIS These two examples are from "Oil and Gas; and Helium
					Production Potential of Oil and Gas Assets in Navajo County,
					Arizona" by Olufela Olukoga, prepared for Blackstone
					Exploration Company Inc.
 
					  
					   Left: Ancient gamma ray neutron log in
					helium bearing reservoir in the Tohache Wash Field. Gas in
					the Mississippian was 6.03% helium. Cumulative production
					was 385 Bcf total gas. Neutron deflections to the right are
					low porosity OR inert gas. Right: Borehole compensated sonic
					log in Kerr-McGee #2 Navajo-C well showing the stratigraphic
					position of the helium-bearing reservoir in the Dineh bi
					Keyah Field. Gas in the Devonian ranges from 3.11% to 6.23%
					helium and averages 4.83% helium and produced 1.4 Bcf total. High sonic travel time is high porosity or shale.
 
					  
					 MODERN PETROPHYSICAL 
					ANALYSIS EXAMPLES These examples are from wells that have tested or produced inert gas with helium in economic quantities.
					The analyses were performed for North American Helium Ltd
					and are reproduced here with their permission.
 
 EXAMPLE 1: Air-drilled Inert Gas Well
 
					
  Left hand tracks contain gamma ray, deep resistivity, density, neutron
					(with gas crossover shaded pink) curves. Right hand tracks
					show calculated effective porosity (with inert gas volume
					shaded red), water saturation, and permeability, Neutron log
					reads zero porosity since inert gas has no hydrogen content
					and there is no invasion from a liquid borehole fluid. SP,
					shallow resistivity, and sonic are missing as they cannot be
					recorded in an air-drilled hole.(Image courtesy NA Hrliun).
 
					
					EXAMPLE 2: Liquid-filled Borehole
 
					  
					
					 Left hand tracks contain gamma ray, deep and shallow
					resistivity, density, neutron (with gas crossover shaded
					pink), PE, and  sonic curves. Neutron log responds to
					invasion water but may read a bit low due to residual inert
					gas in the invaded zone. Right
					hand tracks show calculated effective porosity (with inert
					gas volume shaded red, water saturation, permeability, and lithology analysis. 
					(Image courtesy NA Hrliun).
 
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