Skin Factor and Damage Near Wellbore condition/Skin factor Skin: - damage skin (+) - stimulation (-) - completion skin: - structure skin: - partial completion (+) - slanted (-) - completion: - perforation (+) or (-) - slotted liner (+) - gravel pack - screens Total skin effect: π π π‘π‘ = ∑ π π ππ ο¨ (π π ππ = π π π π π π , π π ππππ , π π ππ ….) Near Wellbore condition/Skin factor Formation Damage Skin : 1. 2. Vertical Well ο¨ Completion Skin : S (+) S (-) Near Wellbore condition/Skin factor * Muskat Model: ππππ = 2ππππβπ€π€ βππ 1 + 7 ∗ ππππ = π π ππ = ππππ ππππ πππ€π€ ππ ππππππ ππππ π€π€ πππ€π€ log ππβπ€π€ 2β 2βπ€π€ 2πππππβππ ππ ππ ππππ ππππ + π π ππ π€π€ 1+7 ∗ β βπ€π€ πππ€π€ log ππβπ€π€ 2β 2βπ€π€ Near Wellbore condition/Skin factor * Papatzacos Model (Anisotropy, Iani = β βπΌπΌ βπ€π€ π π ππ = πππ―π― πππ½π½ ): 1 ππ 1 βπ€π€π€π€ π΄π΄ − 1 − 1 ππππ + ππππ 2 + βπ€π€π€π€ π΅π΅ − 1 βπ€π€π€π€ 2πππ·π· βπ€π€π€π€ Where: π΄π΄ = βπ€π€π€π€ βπ€π€ = β 1 1 π΅π΅ = βπΌπΌπΌπΌ + 3οΏ½4 βπ€π€π€π€ β βπΌπΌπΌπΌ + π€π€π€π€ 4 βπΌπΌπΌπΌ βπΌπΌ = β πππ·π· = πππ€π€ πΌπΌ β ππππππ Near Wellbore condition/Skin factor 2.2 Inclined (or Slanted ) Well Skin Factor: β ππ Where: πΎπΎ = EXAMPLE! 1 πΌπΌππππππ + ππππππ 2 ππ 1− 1 2 πΌπΌππππππ Near Wellbore condition/Skin factor 3. Completion Skin for perforation: TOP VIEW 0°, 360° 180° LATERAL VIEW Before perforation π π π£π£ 120° TOP VIEW π π π€π€π€π€ π π π»π» After perforation 3.1 Perforation skin effect: ππ: phasing ππperf βΆ length of perforation ππππππππππ : perforation radius EXAMPLE! ππθ from table 6.1 4. Combined skin factor of damage and perforation Case 1: πππ π > ππππππππππ + πππ€π€ (π π ππ )ππ πππ π Case 2: πππ π < ππππππππππ + πππ€π€ πππ π ππ = (π π ππ )ππ + π π πππ π ππ ππ π π = π π ππ + π π ππ + (π π ππ )ππ + π π πππ π ππ π π = π π ππ + π π ππ + π π ππ ’ π π π»π» ′ = ππππ πππ€π€ πππ€π€ ′′(ππ) π π ππ ′ = π π ππ ′ +π π π»π» ′ +π π π€π€π€π€ ′ πππ€π€ ′′(ππ) ππππππππππ 4 for ππ = 0 ππππ πππ€π€ + ππ ′ ππππππππ for ππ ≠ 0 1 1 ππππ 2 πππ π βππ = βππ1 + βππ2 ππππ ππππ βππ = ππππ + (π π ππ )ππ πππ€π€ 2πππππ (π π ππ )ππ = ln πππ π πππ€π€ ππππ ππππ βππ1 = ππππ 2πππππ πππ π ππ ππ −1 + π π πππ π πππ π ππ ππππ πππ π βππ2 = ππππ + π π ππ + π π ππ πππ€π€ 2ππππππ β