Xuming Pan, Jing Ba, Rupeng Ma, Weihua Liu, Wei Cheng, José M. Carcione
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Results show that S-wave attenuation decreases with increasing confining pressure, and the water saturation case shows more loss compared to the oil saturation case, while the gas saturation case gives the lowest attenuation. We observe the S-wave relaxation peak at an intermediate water saturation for the gas-water partial-saturation case in general. S-wave attenuation increases with increasing porosity or permeability. Based on the measured rock physical properties, and combined with the Voigt–Reuss–Hill (VRH) average, differential effective medium (DEM) model and squirt-flow model, a tight rock attenuation model is proposed for analyzing the attenuation characteristics of fluid-saturated rocks at different confining pressures. The model reasonably describes the S-wave attenuation characteristics. The model predictions of S-wave attenuation show apparent pressure- and fluid-sensitivity at full saturation and partial saturation conditions. For sample TS1-19 at full saturation with different confining pressures, the S-wave peak attenuation predicted by the model ranges from 11.6 to 69.5, and decreases with confining pressure, while the relaxation frequency shifts to high frequency end. For the partial saturation condition of the sample, the predicted S-wave peak attenuation ranges from 15.5 to 39.8 at a confining pressure of 30 MPa and increases with water saturation, while the relaxation frequency shifts to low frequency end. For all the samples at 30MPa confining pressure, the predicted S-wave attenuation ranges from 5.6 to 38.6. At the full-saturation case, the predicted S-wave attenuation increases with porosity and decreases with confining pressure. For the partial saturation case, the S-wave attenuation predicted with the model and the Voigt and Reuss bounds generally increases with water saturation, whereas the experimentally-measured attenuation exhibits the peak attenuation at an intermediate saturation.</p>","PeriodicalId":55500,"journal":{"name":"Applied Geophysics","volume":"29 1","pages":""},"PeriodicalIF":0.7000,"publicationDate":"2024-01-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Effects of pressure and fluid properties on S-wave attenuation of tight rocks based on ultrasonic experiments\",\"authors\":\"Xuming Pan, Jing Ba, Rupeng Ma, Weihua Liu, Wei Cheng, José M. 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Results show that S-wave attenuation decreases with increasing confining pressure, and the water saturation case shows more loss compared to the oil saturation case, while the gas saturation case gives the lowest attenuation. We observe the S-wave relaxation peak at an intermediate water saturation for the gas-water partial-saturation case in general. S-wave attenuation increases with increasing porosity or permeability. Based on the measured rock physical properties, and combined with the Voigt–Reuss–Hill (VRH) average, differential effective medium (DEM) model and squirt-flow model, a tight rock attenuation model is proposed for analyzing the attenuation characteristics of fluid-saturated rocks at different confining pressures. The model reasonably describes the S-wave attenuation characteristics. The model predictions of S-wave attenuation show apparent pressure- and fluid-sensitivity at full saturation and partial saturation conditions. For sample TS1-19 at full saturation with different confining pressures, the S-wave peak attenuation predicted by the model ranges from 11.6 to 69.5, and decreases with confining pressure, while the relaxation frequency shifts to high frequency end. For the partial saturation condition of the sample, the predicted S-wave peak attenuation ranges from 15.5 to 39.8 at a confining pressure of 30 MPa and increases with water saturation, while the relaxation frequency shifts to low frequency end. For all the samples at 30MPa confining pressure, the predicted S-wave attenuation ranges from 5.6 to 38.6. At the full-saturation case, the predicted S-wave attenuation increases with porosity and decreases with confining pressure. 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引用次数: 0
摘要
中国致密油气藏具有低孔隙度、低渗透率、地层岩石异质性明显等特点,勘探前景广阔,生产潜力巨大。如何理清储层波响应与岩石物性之间的关系仍然是一个挑战,对致密储层波响应模式的深入研究迫在眉睫。岩石的剪切模量和 S-(剪切)波衰减受孔隙流体性质和约束压力的影响。我们对八个部分饱和致密砂岩样品在不同约束压力下进行了超声波实验,并采用频谱比值法估算了 S 波衰减。结果表明,S 波衰减随封闭压力的增加而减小,与油饱和情况相比,水饱和情况下的衰减更大,而气饱和情况下的衰减最小。我们观察到,一般情况下,在气水部分饱和情况下,S 波弛豫峰值处于中间水饱和度。S 波衰减随着孔隙度或渗透率的增加而增加。根据测得的岩石物理特性,结合 Voigt-Reuss-Hill (VRH) 平均法、差分有效介质 (DEM) 模型和喷流模型,提出了一种致密岩石衰减模型,用于分析不同约束压力下流体饱和岩石的衰减特征。该模型合理地描述了 S 波衰减特征。模型预测的 S 波衰减在完全饱和和部分饱和条件下显示出明显的压力和流体敏感性。对于不同封闭压力下完全饱和的 TS1-19 样品,模型预测的 S 波峰值衰减范围为 11.6 至 69.5,并随封闭压力的增加而减小,同时弛豫频率向高频端移动。对于部分饱和条件下的样品,在 30 兆帕的约束压力下,预测的 S 波峰值衰减范围为 15.5 至 39.8,并随水饱和度的增加而增加,同时弛豫频率向低频端移动。在 30MPa 约束压力下,所有样品的预测 S 波衰减在 5.6 到 38.6 之间。在全饱和情况下,预测的 S 波衰减随孔隙度的增加而增加,随约束压力的增加而减小。在部分饱和情况下,根据模型以及 Voigt 和 Reuss 边界预测的 S 波衰减一般随水饱和度的增加而增加,而实验测量的衰减在中间饱和度时达到峰值。
Effects of pressure and fluid properties on S-wave attenuation of tight rocks based on ultrasonic experiments
The tight oil/gas reservoirs in China have showed the great exploration prospects and high production potential, with the characteristics of low porosity, low permeability, and significant heterogeneity in formation rocks. It remains a challenge to sort out the relations between reservoir wave responses and rock physical properties, and the further studies on the wave response patterns of tight reservoirs are in an urgent demand. The shear modulus and S- (shear) wave attenuation of rocks are affected by the properties of pore fluid and confining pressure. The ultrasonic wave experiments are performed on eight partially-saturated tight sandstone samples at different confining pressures, and we estimate S-wave attenuation with the spectral-ratio method. Results show that S-wave attenuation decreases with increasing confining pressure, and the water saturation case shows more loss compared to the oil saturation case, while the gas saturation case gives the lowest attenuation. We observe the S-wave relaxation peak at an intermediate water saturation for the gas-water partial-saturation case in general. S-wave attenuation increases with increasing porosity or permeability. Based on the measured rock physical properties, and combined with the Voigt–Reuss–Hill (VRH) average, differential effective medium (DEM) model and squirt-flow model, a tight rock attenuation model is proposed for analyzing the attenuation characteristics of fluid-saturated rocks at different confining pressures. The model reasonably describes the S-wave attenuation characteristics. The model predictions of S-wave attenuation show apparent pressure- and fluid-sensitivity at full saturation and partial saturation conditions. For sample TS1-19 at full saturation with different confining pressures, the S-wave peak attenuation predicted by the model ranges from 11.6 to 69.5, and decreases with confining pressure, while the relaxation frequency shifts to high frequency end. For the partial saturation condition of the sample, the predicted S-wave peak attenuation ranges from 15.5 to 39.8 at a confining pressure of 30 MPa and increases with water saturation, while the relaxation frequency shifts to low frequency end. For all the samples at 30MPa confining pressure, the predicted S-wave attenuation ranges from 5.6 to 38.6. At the full-saturation case, the predicted S-wave attenuation increases with porosity and decreases with confining pressure. For the partial saturation case, the S-wave attenuation predicted with the model and the Voigt and Reuss bounds generally increases with water saturation, whereas the experimentally-measured attenuation exhibits the peak attenuation at an intermediate saturation.
期刊介绍:
The journal is designed to provide an academic realm for a broad blend of academic and industry papers to promote rapid communication and exchange of ideas between Chinese and world-wide geophysicists.
The publication covers the applications of geoscience, geophysics, and related disciplines in the fields of energy, resources, environment, disaster, engineering, information, military, and surveying.