Submit manuscript...
International Journal of
eISSN: 2475-5559

Petrochemical Science & Engineering

Research Article Volume 2 Issue 5

Determination of Shale Types using Well Logs

Ghassem Alaskari MK,1 Roozmeh A1

1Department of Petroleum Engineering, Petroleum University of Technology, Iran
1Department of Petroleum Engineering, Petroleum University of Technology, Iran

Correspondence: Ghassem Alaskari MK, Department of Petroleum Engineering, Petroleum University of Technology, Iran

Received: February 01, 2017 | Published: June 27, 2017

Citation: Ghassem AMK, Roozmeh A. Determination of shale types using well logs. Int J Petrochem Sci Eng. 2017;2(5):160-166. DOI: 10.15406/ipcse.2017.02.00051

Download PDF

Abstract

Determination of shale type in shale formation has long been a difficult task. Presence of shales in some of the Iranian reservoir formations are one of the most important subject. Shale types have to be considered, because existence of shale type reduces, effective porosity and permeability of the reservoir to some extent. Allogenic Shale is distributed in formations in three basic types, Dispersed, Laminar and structural. Each of these shale types has different effect on porosity, permeability and water saturation. Dispersed shale type reduces effective porosity and permeability to a great extent, but, laminar and structural have less effect on petrophysical parameters. In this investigation, shale types, Shale volume and effective porosity of shale formations have been determined from well logs based on cross-plotting. In other words, a triangle Density-Neutron cross-plot is used to determine the above parameters. The area of study chosen from central oil fields of Iran, where some of the wells are used (Tabnak Field). Tabnak Well C selected for this study in Kangan Formation, South Pars. This study illustrates that distribution of shale types in Kangan Formation is mainly dispersed shale with few of laminar shale, and the quality of effective porosity (φe) decreases with increasing depth in the Kangan Formation.

Keywords: shaley formation, shale types, cross-plotting, kangan formation, well logs

Introduction

Shale is a fine-grained sedimentary rock usually composed of 50% silt (3.9-62.5μm), 35% clay (0.98-3.9μm) and 15% other fine clastic particles (feldspars, quartz, carbonates, zircon, etc.). Shale is distributed in reservoir formations in three basic types, structural, laminar, dispersed or combination of these three types. Each type of shale is described as given in Ghorab.1

Structural shale

Exists in the form of fragments or crystals which are an integral part of the rock framework. In other words, is considered as a portion of rock matrix. This mode of shale distribution has no effect on porosity or permeability.2

Laminar shale

Exists as layer of clay minerals within clean formations (i.e. sandstone, carbonate, etc). The effect of this type on porosity and permeability is sometimes severe and should be investigated.

Dispersed shale

Dispersed shale is composed of clay minerals, fragments or crystals which usually found on grain surface, occupying pore spaces between particles. Dispersed shale will include both detritus and diagenetic clay minerals. One or both of these forms may be present in this type shale. This type of shale reduces effective porosity and permeability to a great extent.

Considerable portion of shale consists of clay minerals such as illite, kaolinite, chlorite, montmorillonite, and etc. Clay minerals in reservoir formation have severe effects on petrophysical properties and reduce the effective and total porosities as well as permeability of the reservoir. Also, shale causes serious problems in formation evaluation and drilling operations.3

Shale affects all well logging measurements to some degree.4 With using well logging data, presence of shale in a formation can be recognized. Besides, shale types, shale volume and effective porosity can be determined either graphically (Cross-plotting) or analytically using Gamma ray spectrum (CGR).

Methodology

In this investigation, Vsh estimated from cross-plot method is compared with Vsh calculated from Gamma ray spectrum (CGR).

Shale volume (Vsh) calculated from gamma ray spectrum

In this paper, Vsh estimated from cross-plot method is validated with Vsh calculated from Gamma ray spectrum (CGR). CGR is the best and most accurate method for determining shale volume. The following equations are used to calculate shale volume.

I G R = C G R log C G R min C G R max C G R min ,         C G R = A log t h + B L o g K MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqzGeGaamysai aadEeacaWGsbGaeyypa0tcfa4aaSaaaOqaaKqzGeGaam4qaiaadEea caWGsbqcfa4aaSbaaSqaaKqzGeGaciiBaiaac+gacaGGNbaaleqaaK qzGeGaeyOeI0Iaam4qaiaadEeacaWGsbqcfa4aaSbaaSqaaKqzGeGa ciyBaiaacMgacaGGUbaaleqaaaGcbaqcLbsacaWGdbGaam4raiaadk fajuaGdaWgaaWcbaqcLbsaciGGTbGaaiyyaiaacIhaaSqabaqcLbsa cqGHsislcaWGdbGaam4raiaadkfajuaGdaWgaaWcbaqcLbsaciGGTb GaaiyAaiaac6gaaSqabaaaaKqzGeGaaiilaabaaaaaaaaapeGaaiiO aiaacckacaGGGcGaaiiOaiaadoeacaWGhbGaamOuaiabg2da9iaadg eaciGGSbGaai4BaiaacEgacaWG0bGaamiAaiabgUcaRiaadkeacaWG mbGaam4BaiaadEgacaWGlbaaaa@6D03@

  1. IGR is the Gamma ray index
  2. CGlog is the Gamma ray spectrum in the zone of interest
  3. CGRmin is the Gamma ray spectrum in cleanest formation
  4. CGRmax is the Gamma ray spectrum in shale zone
  5. A and B are Log calibration constants

Then, the shale volume (Vsh) can be calculated from the Gamma ray index, by the following formula;

Vsh = 0.33[2(2×IGR)-1.0] for hard formation ………… (2)
Vsh =0.083[2(3.7×IGR)-1.0] for soft formation …………. (3)
Vsh =IGR / [3-2IGR] for gas saturated formation [4]……….(4)

Hydrocarbon correction

More accurate method to correct for hydrocarbon effect on density and neutron porosities before points are plotted on cross-plot are given below:6

For the neutron porosity

φ N c o r r =   φ N   Δ φ N MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaape GaeqOXdO2damaaBaaaleaajugWa8qacaWGobGaam4yaiaad+gacaWG YbGaamOCaaWcpaqabaGcpeGaeyypa0JaaeiiaiabeA8aQ9aadaWgaa WcbaqcLbmapeGaamOtaaWcpaqabaGcpeGaai4eGiaabccacqqHuoar cqaHgpGApaWaaSbaaSqaaKqzadWdbiaad6eaaSWdaeqaaaaa@4ADB@ ……………… (5)

Where

Δ φ N = φ S h r ρ h 0.7 + 0.4 P 1 0.4 P MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabfs5aej abeA8aQnaaBaaabaqcLbmacaWGobaajuaGbeaacqGH9aqpcqaHgpGA caWGtbWaaSbaaeaajugWaiaadIgacaWGYbaajuaGbeaadaWcaaqaai abeg8aYnaaBaaabaqcLbmacaWGObaajuaGbeaacqGHsislcaaIWaGa aiOlaiaaiEdacqGHRaWkcaaIWaGaaiOlaiaaisdacaWGqbaabaGaaG ymaiabgkHiTiaaicdacaGGUaGaaGinaiaadcfaaaaaaa@53E4@ For oil…………. (6)
Δ φ N = φ S h r 2.2 ρ h 0.7 + 0.4 P 1 0.4 P MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabfs5aej abeA8aQnaaBaaabaqcLbmacaWGobaajuaGbeaacqGH9aqpcqaHgpGA caWGtbWaaSbaaeaajugWaiaadIgacaWGYbaajuaGbeaadaWcaaqaai aaikdacaGGUaGaaGOmamaaBaaabaqcLbmacqaHbpGCcaWGObaajuaG beaacqGHsislcaaIWaGaaiOlaiaaiEdacqGHRaWkcaaIWaGaaiOlai aaisdacaWGqbaabaGaaGymaiabgkHiTiaaicdacaGGUaGaaGinaiaa dcfaaaaaaa@560E@ For gas …………… (7)

In fresh mud (less than 50000 ppm) the equation can be reduced to:

Δ φ N = φ S h r ( ρ h 0.7 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabfs5aej abeA8aQnaaBaaabaqcLbmacaWGobaajuaGbeaacqGH9aqpcqaHgpGA caWGtbWaaSbaaeaajugWaiaadIgacaWGYbaajuaGbeaacaGGOaGaeq yWdiNaamiAaiabgkHiTiaaicdacaGGUaGaaG4naiaacMcaaaa@4AC8@
Δ φ N = φ S h r ( 2.2. ρ h 1.0 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabfs5aej abeA8aQnaaBaaabaqcLbmacaWGobaajuaGbeaacqGH9aqpcqaHgpGA caWGtbWaaSbaaeaajugWaiaadIgacaWGYbaajuaGbeaacaGGOaGaaG Omaiaac6cacaaIYaGaaiOlaiabeg8aYjaadIgacqGHsislcaaIXaGa aiOlaiaaicdacaGGPaaaaa@4D9E@ for gas…………. (9)

and
Pis salinity of the mud in PPM
φN is neutron porosity
φNcorr is corrected neutron porosity
ρhis hydrocarbon density
Shris residual oil saturation

For the density porosity

φ d c o r r = φ d Δ φ d MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabeA8aQj aadsgacaWGJbGaam4BaiaadkhacaWGYbGaeyypa0JaeqOXdOMaamiz aiabgkHiTiabfs5aejabeA8aQjaadsgaaaa@458E@ ………. (10)

Where,

φ d =   ( ρ m a ρ b ) / ( ρ m a ρ f ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabeA8aQn aaBaaabaqcLbmacaWGKbaajuaGbeaacqGH9aqpqaaaaaaaaaWdbiaa cckacaGGOaGaeqyWdi3aaSbaaeaajugWaiaad2gacaWGHbaajuaGbe aacqGHsislcqaHbpGCdaWgaaqaaKqzadGaamOyaiaacMcaaKqbagqa aiaac+cacaGGOaGaeqyWdi3aaSbaaeaajugWaiaad2gacaWGHbaaju aGbeaacqGHsislcqaHbpGCdaWgaaqaamaaBaaabaqcLbmacaWGMbaa juaGbeaacaGGPaaabeaaaaa@569C@ …………… (11)
Δ φ d =   1.07 φ S h r ( 1.11 ( 1 ρ h ) + 0.65 P 0.03 ) ρ m a 1.0 0.7 P MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabfs5aej abeA8aQnaaBaaabaqcLbmacaWGKbaajuaGbeaacqGH9aqpqaaaaaaa aaWdbiaacckacaaIXaGaaiOlaiaaicdacaaI3aGaeqOXdOMaam4uam aaBaaabaqcLbmacaWGObGaamOCaaqcfayabaWaaSaaaeaacaGGOaGa aGymaiaac6cacaaIXaGaaGymaiaacIcacaaIXaGaeyOeI0IaeqyWdi 3aaSbaaeaajugWaiaadIgajuaGcaGGPaGaey4kaSIaaGimaiaac6ca caaI2aGaaGynaiaadcfacqGHsislcaaIWaGaaiOlaiaaicdacaaIZa GaaiykaaqabaaabaGaeqyWdi3aaSbaaeaajugWaiaad2gacaWGHbaa juaGbeaacqGHsislcaaIXaGaaiOlaiaaicdacqGHsislcaaIWaGaai OlaiaaiEdacaWGqbaaaaaa@68AB@ …for oil…….. (12)
Δ φ d =   1.07 φ S h r 1.11 0.65 P 1.24 ρ h ρ m a 1.0 0.7 P MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabfs5aej abeA8aQnaaBaaabaqcLbmacaWGKbaajuaGbeaacqGH9aqpqaaaaaaa aaWdbiaacckacaaIXaGaaiOlaiaaicdacaaI3aGaeqOXdOMaam4uam aaBaaabaqcLbmacaWGObGaamOCaaqcfayabaWaaSaaaeaacaaIXaGa aiOlaiaaigdacaaIXaGaeyOeI0IaaGimaiaac6cacaaI2aGaaGynai aadcfacqGHsislcaaIXaGaaiOlaiaaikdacaaI0aGaeqyWdi3aaSba aeaajugWaiaadIgaaKqbagqaaaqaaiabeg8aYnaaBaaabaqcLbmaca WGTbGaamyyaaqcfayabaGaeyOeI0IaaGymaiaac6cacaaIWaGaeyOe I0IaaGimaiaac6cacaaI3aGaamiuaaaaaaa@6460@ … for gas…… (13)

In salinity less than 50000 ppm (fresh mud) the parameter, P can be considered zero. An estimation of hydrocarbon density ρh can be obtained by the following equations.

ρ h = 0.7 × ( 1 + φ n φ d ) S h r ( 1 φ n φ d ) ( 1 + 0.72 φ n φ d ) S h r MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabeg8aYn aaBaaabaGaamiAaiabg2da9aqabaWaaSaaaeaacaaIWaGaaiOlaiaa iEdacqGHxdaTdaqadaqaaiaaigdacqGHRaWkdaWcaaqaaiabeA8aQn aaBaaabaGaamOBaaqabaaabaGaeqOXdO2aaSbaaeaacaWGKbaabeaa aaaacaGLOaGaayzkaaGaam4uamaaBaaabaGaamiAaiaadkhacqGHsi slcaGGOaGaaGymaiabgkHiTmaalaaabaGaeqOXdO2aaSbaaeaacaWG UbaabeaaaeaacqaHgpGAdaWgaaqaaiaadsgaaeqaaaaacaGGPaaabe aaaeaacaGGOaGaaGymaiabgUcaRiaaicdacaGGUaGaaG4naiaaikda daWcaaqaaiabeA8aQnaaBaaabaGaamOBaaqabaaabaGaeqOXdO2aaS baaeaacaWGKbaabeaaaaGaaiykaiaadofadaWgaaqaaiaadIgacaWG Ybaabeaaaaaaaa@6246@ for oil saturated………. (14)
ρ h = ( 1 + 0.72 φ n φ d ) S h r ( 1 φ n φ d ) ( 2.2 + 0.8 φ n φ d ) S h r MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabeg8aYn aaBaaabaGaamiAaiabg2da9aqabaWaaSaaaeaadaqadaqaaiaaigda cqGHRaWkcaaIWaGaaiOlaiaaiEdacaaIYaWaaSaaaeaacqaHgpGAda Wgaaqaaiaad6gaaeqaaaqaaiabeA8aQnaaBaaabaGaamizaaqabaaa aaGaayjkaiaawMcaaiaadofadaWgaaqaaiaadIgacaWGYbGaeyOeI0 IaaiikaiaaigdacqGHsisldaWcaaqaaiabeA8aQnaaBaaabaGaamOB aaqabaaabaGaeqOXdO2aaSbaaeaacaWGKbaabeaaaaGaaiykaaqaba aabaGaaiikaiaaikdacaGGUaGaaGOmaiabgUcaRiaaicdacaGGUaGa aGioamaalaaabaGaeqOXdO2aaSbaaeaacaWGUbaabeaaaeaacqaHgp GAdaWgaaqaaiaadsgaaeqaaaaacaGGPaGaam4uamaaBaaabaGaamiA aiaadkhaaeqaaaaaaaa@619F@ for gas saturated……….(15)

Residual hydrocarbon saturation is used, because the neutron and density tools investigate the flushed zone. The saturation in the flushed zone is calculated based on the Archie’s equation.

S x o = ( a φ m × R m f R x o )     = F R m f R x o     a n d   S h r =   1 S x o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakaadofada WgaaqaaKqzadGaamiEaiaad+gaaKqbagqaaiabg2da9maakaaabaGa aiikamaalaaabaGaamyyaaqaaiabeA8aQnaaCaaabeqaaKqzadGaam yBaaaaaaaajuaGbeaacqGHxdaTdaWcaaqaaiaadkfadaWgaaqaaKqz adGaamyBaiaadAgaaKqbagqaaaqaaiaadkfadaWgaaqaaKqzadGaam iEaiaad+gaaKqbagqaaaaacaGGPaaeaaaaaaaaa8qacaGGGcGaaiiO aiabg2da9maakaaabaWaaSaaaeaacaWGgbGaamOuamaaBaaabaqcLb macaWGTbGaamOzaaqcfayabaaabaGaamOuamaaBaaabaqcLbmacaWG 4bGaam4BaaqcfayabaaaaaqabaGaaiiOaiaacckacaWGHbGaamOBai aadsgacaGGGcGaam4uamaaBaaabaqcLbmacaWGObGaamOCaaqcfaya baGaeyypa0JaaiiOaiaaigdacqGHsislcaWGtbWaaSbaaeaajugWai aadIhacaWGVbaajuaGbeaaaaa@6F3C@ ……………… (16)

φis porosity of the formation
m is cementation factor
a is lithology constant
Rmf is resistivity of mud filtrate
Rxois resistivity of flushed zone (micro resistivity tool response)

Shale volume (Vsh) Estimated from cross-plot (CP)

Generally, cross-plot is a quick and commodious method for estimation of shale volume and shale types with acceptable accuracy in comparison with other methods, such as core and log analysis.7 XRD is one the exact methods for clay mineral determination.8

In this cross-plot three distinct points (F, M, SH) are shown Figure 1. Point F represents fluid or water point, where φD= φN=100%. Point M represents matrix point. If density and neutron tools are calibrated in term of the existing matrix, then φN= φD=0. Point SH represents shale point. The coordinate of point SH [φNSh , φDSh] must be determined for shaley portion of well and this coordinate vary from well to well and have to be estimated for each case.9

Figure 1: Triangle neutron-density porosity cross-plot.

Effective Porosity (φe) estimated from cross-plot (CP)

Line M-F represents clean formation or Vsh=0 line. This line is scaled in effective porosity as shown in Figure 1. Points representing φNand φDvalues in clean formations will fall on M-F line and their position on the line indicate effective porosity values. Line M-SH represents φe=0 line and value of each point on this line indicates shale volume of the formation that has no effective porosity. Points that represent shaley formation fall within triangle. Because porosity values do not exceed 50%, line M-F is plotted till 50% porosity to make full use of cross-plot.10 Following equations have been used to construct this triangle.

φ e =   φ n   ( φ N S h .   V s h ) ,       φ e =   φ d     ( φ D s h .     V s h ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaKqbakabeA8aQn aaBaaabaqcLbmacaWGLbaajuaGbeaacqGH9aqpqaaaaaaaaaWdbiaa cckapaGaeqOXdO2aaSbaaeaajugWaiaad6gaaKqbagqaaiabgkHiT8 qacaGGGcGaaiikaiabeA8aQnaaBaaabaqcLbmacaWGobGaam4uaiaa dIgacaGGUaaajuaGbeaacaGGGcGaamOvamaaBaaabaqcLbmacaWGZb GaamiAaaqcfayabaGaaiykaiaacYcacaGGGcGaaiiOaiaacckacqaH gpGAdaWgaaqaaKqzadGaamyzaaqcfayabaGaeyypa0JaaiiOaiabeA 8aQnaaBaaabaqcLbmacaWGKbaajuaGbeaacaGGGcGaeyOeI0IaaiiO aiaacIcacqaHgpGAdaWgaaqaaKqzadGaamiraiaadohacaWGObqcfa OaaiOlaiaacckacaGGGcGaamOvamaaBaaabaqcLbmacaWGZbGaamiA aaqcfayabaGaaiykaaqabaaaaa@73BC@ ………………… (17)

In Figure 1 laminar shale points fall on LAM or around LS-SH line, dispersed shale points fall on or around DIS line and structural shale point’s fall on or around STR line.

For each point within triangle Vsh is estimated on M-SH line parallel to clean formation line (diagonal line), and also, φeis determined on clean formation line parallel to M-Sh line. For example point A in Figure 1 represents a shaley formation that has values of φe= 9% and Vsh = 23%. Shale type for this point is dispersed.11

If formation contains hydrocarbon, Neutron and Density porosities have to be corrected before points are plotted, by using the equations (4-17).

Determination of shale types in kangan formation

There are five depths interval selected for this study from Kangan Formation, well-C Figure 2. The results for each interval have been given below.

Figure 2: Location of well-C in Tabnak field.

Depth intervals “2590-2592m”

This interval of formation has considerable volume of shale and saturated with formation water Figure 3. After plotting measured points of this interval on cross-plot Figure 4 is seen that aggregation of points is around laminar shale line. So, distribution mode of shale for this section of formation is laminar. Vsh and φeestimated from cross-plot for each point of this interval are given in Table 1.

Figure 3: Full set log data for 2590-2592m depth interval.

Figure 4: Neutron-density porosity cross-plot for 2590-2592m depth interval.

PHI-N

PHI-D

PHIE-CP

Vsh -CP

0.424

0.122

0.051

0.88

0.417

0.133

0.067

0.83

0.407

0.141

0.079

0.78

0.395

0.145

0.085

0.73

0.375

0.144

0.09

0.67

0.367

0.141

0.088

0.66

0.35

0.137

0.088

0.62

0.339

0.133

0.085

0.6

0.328

0.128

0.081

0.58

0.315

0.123

0.087

0.56

0.309

0.119

0.074

0.56

0.317

0.117

0.07

0.58

0.335

0.12

0.069

0.63

0.355

0.127

0.074

0.67

0.374

0.138

0.082

0.69

0.384

0.148

0.092

0.69

0.387

0.153

0.098

0.68

0.379

0.152

0.098

0.67

0.373

0.144

0.091

0.67

0.371

0.134

0.078

0.69

0.365

0.125

0.067

0.71

Table 1: Vsh and PHIE (φe) estimated from cross-plot (CP) for depth interval 2590-2592m.

Depth intervals “2650.3-2652”

This section has no shale and there is gas in formation Figure 5. So, neutron and density porosities must be corrected for hydrocarbon effect. Figures 6 & 7 shown positions of points before and after correcting hydrocarbon effect for neutron and density porosities on cross-plot and is seen that points fall on clean formation line after hydrocarbon correction. For this interval, φeestimated from cross-plot, corresponds to 15.2 to 16.8 % Table 2 and effective porosity measured with core analysis method is 17.1 to 18.2%. As one can be seen, this result is very close together, and therefore, this method can be applied to estimate effective porosity with acceptable accuracy. Vsh and φedetermined from cross-plot for each point of this interval are given in Table 2.

Figure 5: Full set log data for 2650.3-2652m depth interval.

Figure 6: Neutron-Density porosity cross-plot for 2650.3-2652m depth interval (before gas correction).

Figure 7: Neutron-density porosity cross-plot for 2650.3-2652m depth interval (after gas correction).

PHIN-COR

PHID-COR

PHIE-CP

Vsh -CP

0.127

0.147

0.152

0

0.127

0.148

0.152

0

0.128

0.148

0.153

0

0.127

0.149

0.153

0

0.126

0.149

0.154

0

0.125

0.15

0.155

0

0.124

0.15

0. 156

0

0.124

0.15

0.156

0

0.125

0.151

0.157

0

0.127

0.152

0.158

0

0.13

0.153

0.159

0

0.134

0.156

0.161

0

0.138

0.159

0.164

0

0.141

0.162

0.167

0

0.142

0.163

0.168

0

Table 2: Vsh and PHIE (φe) estimated from cross-plot (CP) for depth interval 2650.3-2652m.

Depth intervals “2718.5-2719.5m”

This interval of formation has intermediate volume of shale and saturated with formation water Figure 8. After plotting measured points of this interval on cross-plot Figure 9 we seen that points occupy the area between laminar and dispersed shale lines. So, distribution mode of shale for this section of formation is combination of laminar and dispersed types. Vsh and φe estimated from cross-plot for each point of this interval and are given in Table 3.

Figure 8: Full set log data for 2718.5-2719.5m depth interval.

Figure 9: Neutron-density porosity cross-plot for 2718.5-2719.5m depth interval.

Depth

PHI-N

PHI-D

PHIE

Vsh -CP

VSH-CGR

2718.5

0.272

0.065

0.017

0.607

0.557

2718.6

0.274

0.072

0.024

0.595

0.604

2718.7

0.272

0.077

0.031

0.574

0.620

2718.8

0.264

0.079

0.036

0.545

0.593

2718.9

0.254

0.079

0.038

0.513

0.534

2719.0

0.244

0.077

0.038

0.489

0.466

2719.1

0.230

0.074

0.038

0.458

0.411

2719.2

0.219

0.071

0.037

0.434

0.376

2719.3

0.214

0.071

0.037

0.422

0.363

2719.4

0.214

0.072

0.038

0.418

0.368

2719.5

0.215

0.074

0.040

0.414

0.384

Table 3: Vsh and PHIE e) estimated from cross-plot for 2718.5-2719.5m depth interval.

With comparing Vsh. estimated from cross-plot method and Vsh calculated from gamma ray (with using of CGR) is seen that these values are very close together for each point Figure 10, therefore, cross-plot method can be used to determine shale volume and effective porosity with acceptable accuracy.

Figure 10: Vsh estimated from cross-plot and Vsh. calculated from -gamma ray spectrum (CGR) for depth interval 2718.5-2719.5m (Accuracy: 94 - 99%).

Depth intervals “2730.5-2731.5m”

This section of formation has intermediate volume of shale and saturated with formation water Figure 11. After plotting measured points of this interval on cross-plot Figure 12 is seen that aggregation of points is around dispersed shale line. So, distribution mode of shale for this section of formation is dispersed. Vsh and φe estimated from cross-plot for each point of this interval and are given in Table 4.

Figure 11: Full set log data for 2730.5-2731.5m depth interval.

Figure 12: Neutron-density porosity cross-plot for 2730.5-2731.5m depth interval.

Depth

NPHI

PHID

PHIE-CP

VSH-CP

VSH-CGR

2730.5

0.142

0.045

0.022

0.286

0.207

2730.6

0.151

0.049

0.024

0.302

0.239

2730.7

0.158

0.052

0.027

0.312

0.270

2730.8

0.162

0.054

0.028

0.319

0.289

2730.9

0.163

0.055

0.029

0.318

0.289

2731.0

0.159

0.054

0.029

0.310

0.272

2731.1

0.154

0.051

0.027

0.301

0.247

2731.2

0.145

0.047

0.024

0.288

0.224

2731.3

0.132

0.041

0.019

0.270

0.205

2731.4

0.117

0.034

0.014

0.243

0.190

2731.5

0.100

0.027

0.011

0.214

0.171

Table 4: Vsh and PHIE (φe) estimated from cross-plot (CP) for 2730.5-2731.5m depth interval.

With comparing Vsh estimated from cross-plot and Vsh calculated from gamma ray (with using of CGR) is seen that these values are very close together for each point Figure 13, therefore, cross-plot method can be used to determine shale volume and effective porosity with acceptable accuracy.12

Figure 13: Vsh estimated from cross-plot and Vsh calculated from gamma ray spectrum (CGR) for 2730.5-2731.5m depth interval (Accuracy: 89.7-97%).

Depth intervals “2743-2744m”

This interval of formation has low volume of shale and saturated with formation water Figure 14. After plotting measured points of this interval on cross-plot Figure 15 we seen that aggregation of points is around dispersed shale line. So, distribution mode of shale for this section of formation is dispersed. Vsh and φe estimated from cross-plot for each point of this interval and are given in Table 5.

Figure 14: Full set log data for 2743-2744m depth interval.

Figure 15: Neutron-density porosity cross-plot for 2743.-2744m depth interval.

Depth

NPHI-COR

PHID-COR

PHIE-CP

VSH-CP

VSH-CGR

2743.0

0.087

0.043

0.033

0.128

0.136

2743.1

0.100

0.048

0.036

0.152

0.155

2743.2

0.112

0.052

0.038

0.174

0.171

2743.3

0.119

0.055

0.040

0.189

0.181

2743.4

0.121

0.056

0.041

0.193

0.184

2743.5

0.118

0.055

0.040

0.186

0.178

2743.6

0.110

0.052

0.038

0.171

0.165

2743.7

0.099

0.047

0.035

0.152

0.146

2743.8

0.088

0.041

0.031

0.136

0.125

2743.9

0.077

0.036

0.026

0.121

0.106

2744.0

0.068

0.032

0.024

0.105

0.090

Table 5: Vsh and PHIE (φe) estimated from cross-plot (CP) for depth interval 2743-2744m.

With comparing Vsh estimated from cross-plot and Vsh calculated from gamma ray (with using of CGR) is seen that these values are very close together for each point Figure 16, therefore, cross-plot method can be used to determine shale volume and effective porosity with acceptable accuracy.

Figure 16: Vsh estimated from cross-plot method and Vsh calculated from gamma ray spectrum (CGR) for depth interval 2743-2744m (Accuracy: 98.5-99.7%).

Results and discussion

This investigation is done for many depth intervals of Tabnak Well C in Kangan Formation, central Iranian oil field. By using distribution of shale types for each interval, shale volume and the effective porosity for each point have been estimated by cross-plotting method. A triangle neutron-density porosity cross-plot has been applied for this purpose.

  1. For data sets used in this investigation the range of accuracy for determining shale volume using CGR and CP are 89.7% to 99.7%.
  2. This study illustrates distribution of shale types in K- Formation mainly dispersed shale with few of laminar shale.
  3. Based on effective porosity estimated in this investigation, reservoir quality decreases with increasing depth in K-Formation.

 Vsh estimated from cross-plot has been validated with Vsh calculated by Gamma ray spectrum using equations (1) and (3) in unsaturated shale and equation (4) in gas saturated shale. Also, φe estimated using cross-plotting method has been compared with φe, measured by well logs. In shaley formations saturated with hydrocarbon, equations (4) to (17) have been used for correction of shale volume and effective porosity. It is seen that, these shale volumes are very close together. Therefore, cross-plotting method can be used to determine shale volume and effective porosity with acceptable accuracy.

Cross-plotting is a quick and commodious method in comparison with other methods, such as core analysis or well logs for determining petrophysical parameters.

This method can be used for any formation which has shaley layers using cross-plotting of φNSh versus φDSh in each depth interval. Shale types should be determined and recalibrated after a few well has been drilled. The results of this method can be used to estimate productivity and capacity of a reservoir.

Conclusion

  1. Cross-plotting method can be used for determination of shale types, shale volume, and effective porosity with acceptable accuracy.
  2. In case of structural shale, correction for effective porosity is not necessary, but depends on type of clay minerals in this shale type.
  3. In case of Laminated and dispersed types corrections for Vsh and PHIE are essential.
  4. In case of gas saturated shale of any type, correction is needed.

Acknowledgements

None.

Conflict of interest

The author declares no conflict of interest.

References

  1. Ghorab M, Ramadan MA, Nouh A. The Relation Between the Shale Origin (Source or non Source) and its Type for Abu Roash Formation at Wadi El- Natrun Area, South of Western Desert, Egypt. Australian Journal of Basic and Applied Sciences. 2008;2(3): 360-371.
  2. Ruhovets N, Fertl WH. Volumes, Types, and Distribution of Clay Minerals in Reservoir Rocks Based on Well Logs. SPE Unconventional Gas Recovery Symposium, Pittsburgh, Pennsylvania, USA; 1982.
  3. Bassiouni Z. Theory, measurement, and interpretation of well logs. Doherty Memorial Fund of AIME, Society of Petroleum Engineers, Texas, USA, 1994.
  4. Serra O. Fundamentals of well-log interpretation. USA: Elsevier Science Publishing Company Inc; 1984.
  5. Stieber S. Pulsed Neutron Capture Log Evaluation - Louisiana Gulf Coast. SPE paper 2961, Fall Meeting of the Society of Petroleum Engineers of AIME. Houston, Texas, USA, 1970.
  6. Brock J. Applied open- Hole log analysis. USA: Gulf publishing company; 1986.
  7. Tiab DC, Donaldson E. Petro physics: Theory and Practice of Measuring Reservoir Rock and Fluid Transport Properties. USA: Gulf Professional Publishing; 2004.
  8. Ghassem Alaskari MK. Petrophysical Lab Testing. Tehran: Institute of Rahenovin; 2016.
  9. Ghassem Alaskari MK. Analysis of Shaley reservoir zones and their effects on logging tools for Interpretation of Reservoir Parameters in Coastal Fars fields of Iran. ICOFC, Iran; 2012.
  10. Bigelow El. Introduction to Wireline Log Analysis. Houston, Western Atlas International, USA; 1992.
  11. Dresser Atlas. Well logging and interpretation techniques. USA: Dresser ind inc; 1982.
  12. Worthington PF.The Evolution of Shaly-sand Concepts in Reservoir Evaluation. The Log Analyst. 1985;26(1):23–40.
Creative Commons Attribution License

©2017 Ghassem, et al. This is an open access article distributed under the terms of the, which permits unrestricted use, distribution, and build upon your work non-commercially.