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					 GAS
				CORRECTIONS IN HEAVY MINERALS in many carbonate reservoirs, and some sandstones with lots
					of heavy minerals, the heavy mineral effect 
					(separation) is offset by the gas effect (crossover) on the
					density neutron log. The net result is that the gas goes
					unnoticed because there is no crossover, and the lithology
					is misinterpreted because the density neutron separation is
					reduced. Observation of the PE curve will point out the
					inconsistency. In the absence of the PE, sample descriptions
					and core data will point out the problem.
 
 IF gas is known to be present but NO
				crossover occurs after shale corrections, this usually means gas
				in dolomite or in a sandstone with lots of heavy minerals.
				First, assume or calculate the matrix density(DENSMAgc) based
			on the PE curve (PE is the only curve unaffected by gas):
 1:
			V1 = (PE - Vsh * PESH - PE2) / (PE1 - PE2)
 2: V2 = 1 - V1
 3: DENSMAgc = V1 * DENS1 + V2 * DENS2
 Where:DENSMAgc =  matrix density for gas correction (kg/m3 or gm/cc)
 DENS1 = matrix density of mineral 1 (kg/m3 or gm/cc)
 DENS2 = matrix density of mineral 2 (kg/m3 or gm/cc)
 PE = measured PE log value of rock mixture
 PE1 = PE of first mineral (fractional)
 PE2 = PE of second mineral (fractional)
 V1 = volume of first mineral (fractional)
 V2 = volume of second mineral (fractional)
 Vsh = volume of shale (fractional)
 
			DENSMAgc can be computed as a continuous curve or used as a zone
                parameter to replace DENSMA in equation 8.
 Apply gas correction:
 
				4: PHIx = –
				PHIdc / (PHInc / 0.8 – 1) / (1 + PHIdc / (0.8 – PHInc)) 
				5: PHIxdn =
				PHIx + KD3 * (0.30 – PHIx) * (DENSMAgc / KD1 – KD2) 
				  
				Where:  KD1 = 1.00 for English units 
				 KD1 = 1000 for
				Metric units 
				 KD2 = 2.65 for
				Sandstone scale log 
				 KD2 = 2.71 for
				Limestone scale log 
				 KD3 = 1.80 for
				Sandstone scale log 
				 KD3 = 2.00 for
				Limestone scale log 
			
				  
				
				 
				 Density Neutron Complex Lithology Crossplot
				- Gas zones with NO crossover. Enter shale corrected data and
				then slide data point to the right until it reaches the line
				representing the matrix density of the reservoir - travel
				parallel to the nearest heavy black line. Do not use Dolomite scale log for this special
				case.    
                An illustration of how the points move under different conditions
                is given below. 
				 Graph for Gas Correction on Density Neutron Crossplot Porosity,
				showing how the raw data points
 move under various assumptions. (Porosity scales are in Limestone Units)
 Point A goes to A1, if CNL and DENSMA = 2710 (crossover) goes to A2, if SNP regardless of DENSMA
 goes to A3, if CNL and DENSMA = 2870.
 
 Point B goes to B1, if CNL and DENSMA = 2870 and gas correction
                is IMPOSED
 goes to B2, if CNL and DENSMA = 27l0 and gas correction is IMPOSED
 goes to B3, if CNL and DENSMA = 2650 and gas correction is IMPOSED
 stops at B if gas correction is not imposed or if SNP
 
 Point C goes to C1, if CNL and DENSMA = 2870 and gas correction
                is IMPOSED
 goes to C2, if CNL and DENSMA = 2710 and gas correction is IMPOSED
 stops at C if gas correction not imposed or if SNP
 
 The author is indebted to Jim Hamilton of Dome Petroleum for first
                suggesting this approach to one pass gas corrections. The approach
                has proved extremely successful and has matched core on hundreds
                of projects in many reservoir conditions.
 
			Before the introduction of the photo-electric effect (PE) log
                curve, it was easy for a log analyst to miss a gas filled dolomite
                reservoir. The standard density neutron crossplot would show a
                low porosity limestone, when in fact the zone is a medium porosity
                dolomite. Since the density neutron looks like limestone (curve
                separation is small) and the PE looks like dolomite (PE near 3.0),
                this discrepancy is a red flag that a special case exists. Many
                computer programs will not trigger gas corrections unless density
                neutron crossover is present, and most programs do not contain
                explicit algorithms to handle this special case.
 The illustration below  shows the effect of using this gas
				correction. Notice that computed porosity does not match core
				porosity unless the correct DENSMA is chosen. DENSMA should
				reflect the matrix density of the expected lithology. 
			The correction is usually needed in dolomite or dolomitic sands
                or high porosity shaly sands with low to moderate invasion.
   
				 Effect of DENSMA on density neutron crossplot porosity
				with gas in heavy minerals. Core porosity (square black lines)
				and log analysis porosity (smooth black curves) show a good
				match when DENSMA was set at
 2710 - 2740 kg/m3. Log analysis shows near zero porosity if
				DENSMA set at 2650 for this heavy sandstone.
 
				  
				 Gas in dolomite example with
				no correction applied (left) and after correction (rig
 
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