Gambarnya nanti aku bikin dulu dalam pdf supaya tidak kebesaran utk =20 mail attachments RDP =2D--------- | From: Franciscus.Sinartio / mime, , , Franciscus_Sinartio@xxxxxxxxxxx= =2Ecom | To: fogri / mime, , , fogri@xxxxxxxxxxxxx | Subject: [fogri] Re: S wave -seismic multicomponent | Date: Monday, 10 December, 2001 11:55AM | | | | | Vick, | tolong di usahakan supaya kita bisa baca file nya PHN dong.... thank= s | sebelumnya... =3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D for September 2001 ... The Geophysical Corner is a regular column in the EXPLORER, edited by =20 R. Randy Ray. This month's column is titled "Multi-Component, =20 Time-Lapse Seismology for Monitoring Reservoir Production Processes." S-Waves Detect Reservoir Flows Improving reservoir performance and enhancing hydrocarbon recovery are =20 critical to the future of the petroleum industry -- and to do this, it =20 must be possible to characterize reservoir parameters, including fluid =20 properties, their movement and pressure changes with time. Multi-component, time-lapse seismology has great potential for =20 monitoring fluid movements in reservoirs. The main reason is simply the = =20 presence of fluid-filled fractures. Shear waves (S-waves) are much more sensitive than compressional waves =20 (P-waves) to the presence of fractures or microfractures and the fluid =20 content within the fracture network. Seismic shear wave anisotropy in =20 the reservoir causes two shear modes to form (S1 and S2) and to =20 propagate with different velocities. The faster mode (S1) propagates with its particle motion parallel to =20 the open fracture direction, perpendicular to the minimum horizontal =20 stress (S3) in the reservoir -- a phenomenon called S-wave splitting, =20 or birefringence (Figure 1). Seismic shear wave anisotropy is key to monitoring fluid property =20 changes in fractured media. Figure 1. Shear-wave polarization and splitting in a fractured material. As an =20 S-wave with an arbitrary polarization direction enters an anisotropic =20 material, the wave splits into S1 and S2 components with different =20 polarizations and different velocities. The wave polarized parallel to =20 the fractures travels faster and is less attenuated that the wave =20 polarized perpendicular to the fractures. After the S-waves emerge from = =20 the anisotropic material, they continue to propagate as two S-waves =20 with different polarization directions. First 4-D, 9-C Seismic Survey The first time-lapse (4-D), multi-component (9-C) seismic surveys were =20 acquired at Vacuum Field in Lea County, N.M. At the Vacuum Field, shear wave (S-wave) and compressional wave =20 (P-wave) seismic data were used to monitor reservoir fluid property =20 changes associated with a carbon dioxide (CO2) tertiary flood in the =20 Permian San Andres Carbonate. Reservoir fluid properties -- including =20 viscosity, density, saturation and pressure changes -- occur in =20 response to CO2 injection. Changes are caused by CO2 and oil becoming a = =20 miscible phase with the oil in place. These fluid property changes alter the interval velocity and =20 attenuation of S-waves passing through the reservoir interval by up to =20 10 percent, but cause little (1 to 2 percent) or no measurable change =20 in P-wave velocity and attenuation on the surface seismic data. The Reservoir Characterization Project of the Colorado School of Mines =20 (RCP) has conducted two studies at Vacuum Field: =B7 Phase I efforts centered on monitoring the injection of CO2 from a =20 single wellbore (Benson and Davis, 2000). =B7 Phase II is the dynamic reservoir characterization of a six-well CO2= =20 injection program, which includes the Phase-I wellbore (producing =20 during Phase-II) (Wehner, et al, 2000). The Vacuum Field was discovered in 1929 with the drilling of the Socony = =20 Vacuum State 1 well in Section 13-T17S-R34E of Lea County. The Vacuum Field produces predominately from the San Andres Formation =20 in a shallow-shelf carbonate depositional setting (Figure 2), which =20 structurally is positioned on the shelf edge of the Permian Basin's =20 Northwest Shelf. The structurally high shelf crest is located just west = =20 of the RCP study area. Porosity and permeability within the productive zones average 11.8 =20 percent and 22.0 md, respectively. The San Andres gross pay zone can reach 600 feet in thickness, and is =20 divided into two main pay zones: Upper and Lower San Andres. The Lovington Sandstone, a silty interval, segregates the two zones. Figure 2. Type log for the Vacuum field area. The San Andres Formation is at an =20 approximate depth of 4,300 feet and is the primary producing formation =20 in the Vacuum Field. Reservoir Characterization At Central Vacuum Unit (CVU), S-wave splitting is the key to monitoring = =20 production processes associated with carbon dioxide (CO2) flooding. Fluid property changes produce variations in the velocities of the =20 split S-waves passing through the reservoir interval. Reservoir fluids =20 change in response to CO2 and oil becoming a miscible phase in the =20 presence of in-situ fluids. Injected CO2 also can create areas of anomalous reservoir pressure. Both fluid and pressure changes are detected by S-wave splitting and =20 velocities, because they are extremely sensitive to the local stress =20 field caused by the natural fracturing in all rocks, especially carbonat= es. Distinguishing Injected CO2 From Injected Water S-wave splitting can distinguish between effective stress changes =20 associated with abnormal fluid pressures and fluid property change. During Phase I of this study, a prominent S-wave splitting anomaly was =20 detected to the south of a cyclic CO2 injection well (CVU 97). This =20 anomaly corresponds to the CO2 flood bank that developed south of this =20 temporary injection well (Figure 3, Phase I). Noticeable around the periphery to this CO2 anomaly are anisotropy =20 anomalies of opposite sign related to offset wells that were used to =20 contain the CO2 bank through water injection. The sign change of S-wave = =20 anisotropy occurs because the relative velocities of the split S-waves r= everse. In the case of the miscible CO2-oil bank, the S2 velocity increased and = =20 S1 decreased, whereas, in the case of water injection, the effective =20 stress causes S2 to decrease and S1 to increase. Similar effects were observed during the second phase of the monitoring = =20 study (Figure 3, Phase II). These results imply that S-wave anisotropy =20 can be used to monitor secondary (water flooding) as well as tertiary =20 (CO2) methods in a spatial context beyond the wellbore. The greatest need of tertiary recovery operations is to monitor and =20 control the areal and vertical distribution of injected CO2 in the =20 reservoir. Controlled injection can maximize contact with the oil and =20 optimize sweep efficiency so that oil is not bypassed. A spatial image of the tertiary flood-front was visualized by observing = =20 time-lapse anisotropy differences. This enables the lateral sweep =20 efficiency of the reservoir to be monitored. The vertical sweep efficiency can be detected through amplitude =20 differentials of split S-waves. S2 amplitude difference anomalies =20 between the pre- and post-surveys occur dominantly in the Lower San =20 Andres. This is highly encouraging, because S-wave anisotropy may =20 provide higher vertical resolution, enabling a visualization of changes = =20 approaching the individual flow-unit scale. The time-lapse seismic interpretation of the Phase II seismic data =20 showed a differential seismic anisotropy anomaly between the baseline =20 and monitoring survey that coincides with the tertiary flood bank =20 (Figure 3, Phase II). This anomaly was measured over the entire =20 reservoir interval, and is shown as a velocity anomaly where S1 =20 velocity decreased and S2 velocity increased. Figure 4 shows the correspondence between time-lapse P-wave velocity, =20 time-lapse S-wave polarization direction and time-lapse S-wave velocity = =20 anisotropy anomalies. Using this information, it is possible to =20 separate the effective stress changes associated with changing fluid =20 pressure from the fluid saturation changes associated with the tertiary = =20 flood bank. As a result, the tertiary flood bank -- and its growth over time -- can = =20 be monitored by this technology. Figure 3. Time-lapse shear-wave velocity anisotropy differences. Phase I) CO2 =20 injection occurred at the CVU-97 well with a prominent S-wave =20 anisotropy anomaly detected to the south. Phase II) CO2 injection =20 occurred at the six offset injectors (indicated by triangles). In the =20 case of the miscible CO2-oil bank, the S2 velocity increased and S1 =20 velocity decreased (purple), whereas, in the case of water injection, =20 the change in effective stress causes the S2 velocity to decrease and =20 S1 velocity to increase (blue). Figure 4. Phase II seismic anomalies. The upper diagram shows the time-lapse =20 P-wave velocity differences while the lower diagram shows the =20 time-lapse S-wave velocity anisotropy differences. Overlain on each =20 diagram are the S-wave polarization direction differences (areas that =20 have changes in the S-wave polarization direction). Areas of the =20 reservoir that have P-wave velocity and S-wave polarization direction =20 anomalies correspond to zones of the reservoir with pressure changes. =20 Areas of the reservoir that have S-wave anisotropy anomalies correspond = =20 to zones with fluid saturation changes. Conclusions The study indicated that shear wave analysis provided higher resolution = =20 (than P-wave data) static reservoir characterization, allowing for =20 visualization of inter-well distribution of secondary porosity, =20 permeability and fracture zones. Due to rigidity changes associated with fluid replacement in the =20 reservoir, dynamic monitoring with shear wave data provided a means to =20 actively follow the displacement of reservoir fluids with CO2. This dynamic reservoir characterization will provide the industry with =20 the ability to be more proactive, rather than reactive, in the =20 management of reservoirs. ---- Gabung Milist Fogri, email ke fogri-request@xxxxxxxxxxxxx dengan subject subscribe Keluar Milist Fogri, email ke fogri-request@xxxxxxxxxxxxx dengan subject unsubscribe homepage : http://www.fogri.f2s.com Archieve : //www.freelists.org/archives/fogri/ -----