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					 Nuclear
					Magnetic LogS Nuclear Magnetic Resonance Logs come in many
					flavours and have been around  for more than 40 years.
					However, they are still quite rare and only the last few
					years have shown themselves to be useful in identifying
					zones with high irreducible water that would be previously
					be considered too wet to be worth completing. By comparing
					irreducible water from NMR with total pore water from
					conventional logs, an estimate of water cut can be made.
					However, results from many NMR calculations are still
					ambiguous.
 The
			chief application of the NMR tool is to determine
			moveable fluid volume (BVM) of a rock. This is the pore space excluding
			clay bound water (CBW) and irreducible water (BVI). Neither of these
			are moveable in the NMR sense, so these volumes are not easily
			observed on older logs. On modern tools, both CBW and BVI
			can often be seen in the signal response after transforming the
			relaxation curve to the porosity domain. Note that some of the
			moveable fluids (BVM) in the NMR sense are not actually moveable in
			the oilfield sense of the word. Residual oil and gas, heavy oil, and
			bitumen may appear moveable to the NMR precession measurement, but
			these will not necessarily flow into a well bore. 
			Micritic interparticle porosity and pin point vugs
			in carbonates may be included in the CBW fraction. This may cause a
			minor difference between effective porosity seen by conventional
			logs and from NMR, especially in clean rocks in which some of the
			porosity has very small pore size.
 With stronger magnets and better processing, modern
			tools can usually give the irreducible water volume (BVI) and clay
			bound water (CBW). Effective porosity (PHIe) is the sum of BVI and
			BVM. In hydrocarbon zones at initial conditions, water saturation is
			BVI divided by PHIe. No shale corrections or resistivity log are
			needed.
 
 The rock volume measured is very small compared to
			density and neutron logs, so there is some possibility for
			inconsistent results when comparing NMR porosity to these sources.
 Unlike many other logging tools,
			the NMR design and operating principles are somewhat different
			between different service suppliers. A Schlumberger CMR tool
			investigates a chunk of rock about the size of a good Cuban cigar,
			about 1 inch from the borehole wall, in front of the permanent
			magnet on the face of the tool.  Halliburton's MRIL tool (NUMAR
			design) measures a thin cylinder about 2 inches inside the rock,
			circling the entire borehole. The Baker Atlas MREX tool sees a 120
			degree segment of a cylinder about 2 inches into the rock. 
			 
			  Measured rock volume for MRIL (red circle), CMR (red dot), and MREX
			(grey)
 
			The NMR is now widely used in unconventional reservoirs as it is
			immune to the effect of organic carbon (kerogen) so the effective
			porosity from NMR needs no further correctiom, unlike sonic,
			density, and neutron log porosity.
 
 
					
					 References: 1. Effective Porosity and Permeability of
			Sandstones Investigated Through Nuclear
 Magnetic Resonance
			Principles
 A. Timur, SPWLA, 1968
 
					
					 LOG RESPONSE
			
			
					
					EQUATION fOR Nuclear
					Magnetic LogS The Log Response Equation for modern nuclear magnetic logs is
                the same as for all other logs. The difference between the NMR
                and other porosity logs is that the Log Response Equation is solved
                by the service company at logging time, instead of by the analyst
                after the logs are delivered. This transform is illustrated
			below.
   
				 Transforming the precession decay time curve into the porosity
			domain, showing breakdown of CBW,
			BVI,
 and BVM.
			The T2 cutoff for the boundary between CBW and BVI is often chosen
				at 3 ms. In sandstones, the boundary between BVI and BVM is
				usually chosen at 32 or 33 ms, but in carbonates the cutoff
				could be much higher (80 to 120 ms) and varies with lithology.
				The cutoffs can be determined on rock samples in the lab.
 
 
    T2 distribution for heavy oil (red curve) and light oil (yellow)
				- area under the curves are equal, so total porosity is
				independent of hydrocarbon density. T2 cutoff between BVI and
				BVM varies with lithology - total porosity does not vary with
				lithology, but BVI and BVM do vary with lithology.
 The
                matrix and dry clay terms of NMR response are zero. As a result
				the NMR porosity is said to be independent of lithology.
				However, this is only true for total porosity (the total area
				under the shaded curve in the above illustration). The boundary
				between CBW and BVI, and the boundary between BVI and BVM, do
				depend on lithology and may vary foot by foot through the
				reservoir. As a result, the choice of fixed T2 cutoff times to
				represent these boundaries is not a good idea, and more
				elaborate methods are now being used. 
			 An NMR log
                run today can display clay bound water (CBW), irreducible water
                (capillary bound water, BVI), and mobile fluids (hydrocarbon plus
                water, BVM), also called free fluids or free fluid index (FFI).
                On older logs, only free fluids (FFI) are recorded and some subtractions,
                based on other open hole logs, are required to obtain BVI and
			CBW. A
			confusion is caused by the term Moveable Fluids or Free Fluids (BVM
			in the diagram above). The freedom to move refers to the protons in
			the fluid, not to the fluid itself. Some or all of the BVM may be
			immoveable, as residual oil, heavy oil, bitumen, or tar. 
			Comparison of
			conventional and NMR porosity shows that effective porosity (curves to the left of the red shading) are nearly identical. Water
			volume from
 PHIe*Sw and BVI are also very similar (right edge of red shading),
			indicating
 that the water is irreducible and not moveable
  
					
					 Porosity from Modern Nuclear
					Magnetic LogS For modern NMR logs:
 1: PHIt = PHIcbw + PHIbvi + PHIbvm
 2: PHIe = PHIbvi + PHIbvm
 3: PHIuse = PHIbvm
 4: SWir = PHIbvi / PHIe
 5: IF SW >> SWir
 6: THEN zone will produce with a water cut
 
 Where:
 PHIcbw = clay bound water (fractional
 PHIbvi = irreducible water or capillary bound water (fractional)
 PHIbvm = mobile fluids (fractional)
 PHIt = total porosity (fractional)
 PHIe = effective porosity (fractional)
 PHIuse = useful porosity (fractional)
 SWir = irreducible water saturation (fractional)
 
			
  Nordegg tight oil shows large separation between the density (red
			curve) and neutron porosity (black short dash), even though the sand
			is clean according to the gamma ray log. The core porosity (blue
			dots) and NMR total porosity (solid grey) are about halfway between
			the two conventional porosity curves, which is where the Complex
			Lithology model would also put the porosity. The PE (black heavy
			dash) varies between 1.8 and 4.5 showing the variable nature of the
			heavy mineral content. 
			NMR porosity is unaffected by organic carbon (TOC)
			so it is a good log in shale gas environments. (image courtesy
			Schlumberger)
 
					
					 COMMENTS Some or all of the sums defined above may be displayed on the
                delivered log. Log presentation is far from standard for NMR logs.
 
 In some situations, mobile water can be separated from hydrocarbon,
                and sometimes gas can be distinguished from oil, by further (experimental)
                processing of the original signal. However, the depth of investigation
                and measurement volume are tiny, so the hydrocarbon indication
                is from the invaded zone.
 
 For the same reason, PHIt and PHIe from NMR do not always agree
                with that derived from density neutron methods, which see much
                larger volumes of rock.
 
 
  RECOMMENDED PARAMETERS None required.
 
			
			
			
			 Porosity from Older Nuclear Magnetic Logs On
			older NMR logs, only free fluids (FFI) are recorded and some subtractions,
                based on other open hole logs, are required to obtain BVI and
			CBW.
 
			
                For older NMR logs: 7: PHInmr = FFI
 8: SWir = KBUCKL / PHInmr
 9: PHIe = FFI / (1 - SWir)
 10: BVWSH = (PHINSH + PHIDSH) / 2
 11: PHIt = PHIe + Vsh * BVWSH
 
 IF  PHIe is known from some other log:
 12: PHIbvi = PHIe - PHInmr
 13: SWir = PHIbvi / PHIe
 
                Where:
 FFI = free fluids or free fluid index (fractional)
 PHInmr = NMR porosity (fractional)
 PHIt = total porosity (fractional)
 PHIe = effective porosity (fractional)
 SWir = irreducible water saturation (fractional)
 Vsh = shale volume (fractional)
 BVWSH = bound water 100%in shale (fractional)
 
 
  COMMENTS PHIe and PHIt should be compared to density neutron or other methods
                defined earlier. The significant difference in measured volume
			between NMR and other logs may give silly answers that need to be
			trimmed or smoothed.
 
 
  RECOMMENDED PARAMETERS KBUCKL is in the range 0.010 to 0.100, with a default of 0.040.
 
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