4.2.1 Seismic forward responses for no reservoir developed
Canglangpu Formation, Longwangmiao Formation and Gaotai Formation in the model are set to constant velocity, and the velocity value is derived from the average formation velocity of the four wells on the north slope, which are 5255 m/s for the Canglangpu Formation, 6772 m/s for the Longwangmiao Formation, and 6096 m/s for the Gaotai Formation. A wedge-shaped model of the Longwangmiao Formation with undeveloped reservoirs is established to observe seismic waveform varying with its stratal thickness (0 ~ 110 m) (Fig. 5a). The thickness of the Canglangpu Formation and Gaotai Formation in the model is relatively thick, which will not affect the waveform of the Longwangmiao Formation.
Combined with the drilling results of the central Sichuan paleo-uplift and the northern slope, the thickness of the Longwangmiao Formation is between 60 m and 130 m. Therefore, we focus on the waveform features of the Longwangmiao Formation with a thickness greater than 60 m in Fig. 5. The results show that the bottom interface of the Longwangmiao Formation constantly corresponds to the extreme value of the wave trough, while the top interface of the Longwangmiao Formation varies with its stratal thickness (Fig. 5b).
i) When the thickness of the Longwangmiao Formation is between 60 m and 90 m (e.g., the thickness of the Longwangmiao Formation is 80 m), the top interface of the Longwangmiao Formation is located about 1/8λ above the wave peak (Fig. 5b).
ii) When the stratal thickness reaches more than 90 m, the waveform of the upper Longwangmiao Formation changes from single peak to double peak gradually. When the stratal thickness is greater than 110 m, the two peaks of double peak are obviously separated (Fig. 5b).
4.2.2 Seismic forward responses for reservoir developed
According to the above, with the different of the stratal thickness, the upper Longwangmiao Formation will produce two types of waveforms, namely single peak and double peak (Fig. 5). Therefore, when the stratal thickness of the Longwangmiao Formation is thin (60 ~ 90 m) and thick (greater than 90 m) and when reservoirs are developed internally, it is necessary to explore the waveform changes corresponding to the Longwangmiao Formation, in order to achieve the purpose of identifying reservoirs through the seismic facies.
(1) Reservoir seismic reflection under thin formation (60 ~ 90 m) background
Under the background of the stratal thickness of 60 m ~ 90 m in the Longwangmiao Formation, a wedge-shaped geological model is established, in which only the upper reservoir (i.e., the reservoir developed in the SMLF) and both the upper and lower reservoirs (i.e., the reservoir developed in the first and second members of the Longwangmiao Formation) are developed (Figs. 6 and 7). The parameters, such as and formation thickness, formation velocity, reservoir thickness and reservoir velocity of the Longwangmiao Formation, are shown in Table 2. By the seismic forward modeling, the results indicate that:
i) When the reservoir is developed in the SMLF, the seismic waveform of the Longwangmiao Formation is still dominated by the skew-symmetrical waveform from the peak to the trough, but the top peak has the characteristics of downward movement (Model 1 in Fig. 6). The downward movement will become more obvious with the decrease of the reservoir velocity of the SMLF, which will eventually lead to the peak located in the middle of the Longwangmiao Formation (Model 2 in Fig. 6). At the same time, as the reservoir velocity decreases, the peak amplitude inside the Longwangmiao Formation will also increase (compared with Models 1, 2 and 4 in Fig. 6). Meanwhile, the top interface of the Longwangmiao Formation is generally located below the upper trough. The lower the reservoir velocity, the stronger the trough amplitude corresponding to the top interface of the Longwangmiao Formation.
ii) When multiple sets of reservoirs are developed in the SMLF, the velocity of each set of reservoirs is set to be consistent with the velocity of a single set of reservoirs, and the cumulative thickness of multiple sets of reservoirs is also consistent with the thickness of a single set of reservoirs. The forward modeling results show that the waveforms of multiple sets of reservoirs are consistent with those of a single set of reservoirs (compared to Models 2 and 3 in Fig. 6).
iii) When reservoirs are developed in both the first and second members of the Longwangmiao Formation, firstly, the reservoir characteristics of the first and second members are set to be identical (i.e., consistent thickness and velocity). Meanwhile, the waveform of the Longwangmiao Formation does not change significantly (Model 1 in Fig. 7). The actual geological conditions do not lead to this situation. Secondly, if the reservoir thickness of the SMLF is greater than that of the first member of the Longwangmiao Formation (Model 2 in Fig. 7), the wave peak will move downward, and as the reservoir velocity decreases, the wave peak will move downward more significantly and the peak amplitude will also increase (Model 3 in Fig. 7). Thirdly, if the reservoir velocity of the SMLF is lower than that of the SMLF, the wave peak moves downward (Model 4 in Fig. 7).
In summary, when the thickness of the Longwangmiao Formation is 70 m ~ 90 m, the reservoir development in the SMLF can be determined by three characteristics: the upper peak of the Longwangmiao Formation moves down into the formation, the middle peak amplitude increases, and the top trough amplitude increases.
(2) Reservoir seismic reflection under thick formation (over 90 m) background
Under the background that the thickness of the Longwangmiao Formation is more than 90 m, a wedge-shaped geological model was established, in which only the upper reservoir (i.e., the reservoir developed in the SMLF) and both the upper and lower reservoirs (i.e., the reservoir developed in the first and second members of the Longwangmiao Formation) are developed (Figs. 8 and 9). The parameters, such as formation thickness, formation velocity, reservoir thickness and reservoir velocity of the Longwangmiao Formation, are shown in Table 2. Using seismic forward modeling, the results are as follows:
i) When reservoirs are developed in the SMLF, the top peak moves down, and the internal peak of the Longwangmiao Formation undergoes interference and merges into a single peak. Currently, the Longwangmiao Formation exhibits a trough-peak-trough reflection from top to bottom (Fig. 8). As the reservoir velocity of the SMLF decreases, the wave peak moves downward more significantly, and the peak amplitude within the formation increases as well (compared to Models 1 and 2 in Fig. 8) and the trough amplitude corresponding to the top interface of the Longwangmiao Formation increases.
ii) When multiple sets of reservoirs are developed in the SMLF, the velocity of each set of reservoirs is set to be consistent with the velocity of a single set of reservoirs, and the cumulative thickness of multiple sets of reservoirs is also consistent with the thickness of a single set of reservoirs (compared to Model 2 and 3 in Fig. 8). The forward modeling results show that the waveforms of multiple sets of reservoirs are consistent with those of a single set of reservoirs, indicating that the cumulative thickness of the reservoir is one of the critical factors affecting the waveform reflection of the reservoir.
iii) When reservoirs are developed in both the first and second members of the Longwangmiao Formation, firstly, the reservoir characteristics of the first and second members of the Longwangmiao Formation are set to be identical (i.e., consistent thickness and velocity). Meanwhile, the top peak of the Longwangmiao Formation moves slightly downward, and the top peak connects with the middle peak to form a low-frequency peak (Model 1 in Fig. 9). Secondly, if the reservoir thickness of the second member in the Longwangmiao Formation is greater than that of the first member of the Longwangmiao Formation, the double peak in the upper Longwangmiao Formation will interfere and merge into a wave peak, and the top peak will move downward (Model 2 in Fig. 9). It should also be noted that the morphology of single peak is an asymmetric low-frequency peak, and the maximum value of the wave peak is close to the middle Longwangmiao Formation. Thirdly, when the reservoir thickness of the SMLF is greater than that of the first member of the Longwangmiao Formation, and the reservoir velocities of the second and members of the Longwangmiao Formation are lower, there is still only a wave peak within the Longwangmiao Formation, but the wave peak moves down more significantly, and the wave peak shape is still asymmetric. The maximum value of the wave peak is close to the upper Longwangmiao Formation (Model 3 in Fig. 9), which is different from Model 2 in Fig. 9. Fourthly, when the reservoir thickness of the second member is equal to that of the first member in the Longwangmiao Formation, but the reservoir velocity of the second member is lower than that of the first member, the wave peak moves downward and the wave peak shape is similar to that of the Model 3 in Fig. 9 (Model 4 in Fig. 9).
Based on the above results, when the thickness of the Longwangmiao Formation is greater than 90 m with the reservoir development, three characteristics can be used to judge the reservoir development in the SMLF: the double peak is merged into single peak, the asymmetric peak moves down into the formation, and the top interface of the Longwangmiao Formation corresponds to the trough.