SU272450A1 - METHOD OF DIELECTRIC ELECTROMAGNETIC CARTRIDGE - Google Patents
METHOD OF DIELECTRIC ELECTROMAGNETIC CARTRIDGEInfo
- Publication number
- SU272450A1 SU272450A1 SU1300463A SU1300463A SU272450A1 SU 272450 A1 SU272450 A1 SU 272450A1 SU 1300463 A SU1300463 A SU 1300463A SU 1300463 A SU1300463 A SU 1300463A SU 272450 A1 SU272450 A1 SU 272450A1
- Authority
- SU
- USSR - Soviet Union
- Prior art keywords
- value
- rocks
- ratio
- distance
- dielectric
- Prior art date
Links
- 239000011435 rock Substances 0.000 description 12
- 238000005259 measurement Methods 0.000 description 4
- 230000035699 permeability Effects 0.000 description 2
- 208000008454 Hyperhidrosis Diseases 0.000 description 1
- WUAPFZMCVAUBPE-UHFFFAOYSA-N Rhenium Chemical compound [Re] WUAPFZMCVAUBPE-UHFFFAOYSA-N 0.000 description 1
- 238000005056 compaction Methods 0.000 description 1
- 230000000875 corresponding Effects 0.000 description 1
- 230000001419 dependent Effects 0.000 description 1
- 238000005553 drilling Methods 0.000 description 1
- 230000005672 electromagnetic field Effects 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 229910052702 rhenium Inorganic materials 0.000 description 1
- 239000000523 sample Substances 0.000 description 1
- 230000035900 sweating Effects 0.000 description 1
Description
Изобретение относитс к промыслово-геофизическим методам исследовани скважин.This invention relates to a geophysical field survey method.
Известен снособ диэлектрического каротажа , при котором диэлектрическую проницаемость горных пород олредел ют путем измерени разности фаз высокочастотного (пор дка дес тков мегагерц) магнитного дол . Высокочастотное магнитное поле возбуждаетс в скважине с помощью вертикального магнитного дипол , разность фаз измер етс меладу двум разнесенными приемными катушками, удаленными на некоторое рассто ние от геператорного дипол . Способ позвол ет исключить или существенно уменьшить вли ние удельного сопротивлени среды (при величине его не менее 20-25 ом-м) на результаты измерений диэлектрической проницаемости горных пород.A dielectric logging method is known, in which the dielectric constant of rocks is determined by measuring the phase difference of a high-frequency (of the order of tens of megahertz) magnetic fraction. The high-frequency magnetic field is excited in the borehole using a vertical magnetic dipole, the phase difference is measured by the malad of two spaced-apart receiving coils, separated by a distance from the hetero-dipole. The method makes it possible to eliminate or substantially reduce the influence of the resistivity of the medium (at a value of at least 20-25 ohm-m) on the results of measurements of the dielectric constant of rocks.
С целью ловышени точности определени электрических свойств горных пород, согласно предлагаемому способу, одновременно с разностьюфаз Аф пол измер ют отношени амплитуд пол в тех же точках, и по резульЛаIn order to gain accuracy in determining the electrical properties of rocks, according to the proposed method, the ratios of the amplitudes of the fields at the same points are measured simultaneously with the difference between the phases of the Af field, and
татам изме;рений вычисл ют значени диэлектрической проницаемости и сопротивлени горных пород.tatam measurements; rhenium calculates the values of dielectric constant and resistance of rocks.
в дол х дол в воздухе определ етс следующим выралсением.In proportion, the proportion in the air is determined by the following compaction.
Л, К(1 + br,Y + (.L, K (1 + br, Y + (.
где аи b - действительна и мнима части волнового числа.where au and b are real and imaginary parts of the wave number.
K. a-{-ib.K. a - {- ib.
На рассто нии га от генераторного дипол ам.плитуда будет равнаAt a distance ha from the generator dipole, the amplitude will be
A, ( + br,f + (ar.Y.A, (+ br, f + (ar.Y.
Отношение амплитуд в двух точках на рассто ни х ri и Га от генератора, учитыва , что /2 г1+Аг, где Аг - рассто ние мелсду приемными катушками, будет равноThe ratio of the amplitudes at two points on the distance x ri and ha from the generator, taking into account that / 2 r1 + Ar, where Ar is the distance to the receiving coils, will be
К(1 + bri) + (ari) А е- У (I + Ьг,, ( K (1 + bri) + (ari) A e- Y (I + Lg ,, (
йдг /(1 -t- briY- + (arif Y(i + + {ar.)Величина отношени - в основном опредеAZ ydg / (1 -t- briY- + (arif Y (i + + {ar.)) The ratio is mainly determined by
л етс членом , характеризующим затухание волны на рассто нии от первой до второй приемной -катушки. Величина b при отношении - 1 опреде/т 2 л етс выражением , 1887 yi проводимость среды, со - частота пол , е относительна диэлектричес 10-9 ка проницаемость S -, 1J, - маг (,зенитна проницаемость среды. Можно .прин ть, что р, |.. Таким образом, величина 6, а следовательно , и отношение - в основном определ ютс величиной -проводимости .пород и в гораздо меньшей мере завис т от величины е. В реальных услови х когда скважина запоЛНена б;; р01вы М {раствароад с удельным сюгоротивлением меньшим, чем сопротивление окружаю Ш ,их потод, отношение - также будет определ тьс затуханием во вмещаюш,их породах на рассто нии между приемными катушками и пра.ктически не будет зависеть от удельного сопротивлени раствора и небольших из.менений диаметра скважины. Это объ сн етс тем, что хот амплитуда пол , наведенного в .каждой из -катушек, зависит от сопротивлени бурового раствора, в отношении это вли ние исключаетс , таК как скважина одинаково вли ет на сигнал в .первой и во второй катушках, поскольку луть волны, .приход щей от источника дол к первой и ко второй приемной катушкам, одина.ков и отличаетс только интервалом во вмещающих породах длиной Дг Г1-Г2. Поскольку измерение отношени - не дает точных значений .проводимости, определение истинного значени s следует проводить с помощью номо.грамм вида, показанного на чертеже . Номогра.мма рассчитана дл частоты 60 Мгц и зонда с рассто ни ми между генераTopoai и приемниками 0,8-и 1 м. На номограмме нанесено два семейства кривых. Одно семейство соответствует разным значени м разности фаз Дф, другое - различным значени .м отношени амплитуд - . Дл о.пределени истинного значени е породы с каротажной диаграммы снимают наблю 1 денные значени Дф и - и на номограмме Л отыскивают точку пересечени соответствующих линий- Дф и - . Абсцисса этой точки харастеризует значение е породы, с оси ординат снимаетс значение р. Таким образом, данный способ позвол ет нар ду с величиной е .определить значение удельного сопротивлени породы на высокой частоте. Предмет изобретени Способ диэлектрического электромагнитного каротажа, заключающийс в возбуждении в скважине электромагнитного пол частотой .пор дка дес тков мегагерц и изьмерений разности фаз пол в двух его точках, отличающийс тем, что, с целью повышени точности определени электрических свойств горных .пород, дополнительно измер ют отношение амплитуд пол в тех же точках и ло результатам измерений вычисл ют значени диэлектрической проницаемости и сопротивлени горных пород.It is a member characterizing the attenuation of the wave at a distance from the first to the second receiving coil. The value of b at the ratio - 1 is determined / m 2 by the expression, 1887 yi is the conductivity of the medium, co is the frequency of the field, it is relative dielectric 10-9 as the permeability S -, 1J, is the mag (, the zenith permeability of the medium. that p, | .. Thus, the value of 6, and hence the ratio, is mainly determined by the value of the conductivity of the rock and is much less dependent on the value of e. In actual practice, when the well is filled b ;; {solution with specific syrupivne less than the resistance surround W, their sweating, attitude - will also be op Determined by the attenuation in space, their rocks at a distance between the receiving coils and in practice will not depend on the specific resistance of the solution and small changes in the borehole diameter. This is due to the fact that although the amplitude of the field induced in each coils depends on the resistance of the drilling fluid, with respect to this influence is excluded, since the well equally affects the signal in the first and second coils, because the wave’s lead coming from the source to the first and the second pick-up coils .kov and distinguishing It is only an interval in the surrounding rocks length Az G1-G2. Since the measurement of the ratio does not give exact conductivity values, the determination of the true value of s should be carried out using a nomogram of the form shown in the drawing. The nomogram is designed for a frequency of 60 MHz and a probe with a distance between the Topoai generator and receivers of 0.8 and 1 m. On the nomogram there are two families of curves. One family corresponds to different values of the phase difference Df, the other to different values of the ratio of amplitudes -. To determine the true value of the rock, the observed values of Df and с are removed from the well log and - and on the nomogram L they find the point of intersection of the corresponding lines - Df and -. The abscissa of this point characterizes the value of rock e, the value of p is taken from the ordinate axis. Thus, this method allows, along with the value of e., To determine the value of the resistivity of the rock at a high frequency. Subject of the Invention A method of dielectric electromagnetic logging, which involves exciting an electromagnetic field in a well with a frequency of about tens of megahertz and measuring the phase difference of the field at its two points, characterized in that, in order to improve the accuracy of determining the electrical properties of rocks, it is also measured the ratio of the amplitudes of the field at the same points and the results of the measurements calculate the dielectric constant and the resistance of the rocks.
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Publications (1)
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SU272450A1 true SU272450A1 (en) |
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Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4009434A (en) * | 1974-12-09 | 1977-02-22 | Texaco Inc. | Dielectric induction logging system for obtaining water and residual oil saturation of earth formations |
US4012689A (en) * | 1974-10-24 | 1977-03-15 | Texaco Inc. | Radio frequency resistivity and dielectric constant well logging utilizing phase shift measurement |
US4052662A (en) * | 1973-08-23 | 1977-10-04 | Schlumberger Technology Corporation | Method and apparatus for investigating earth formations utilizing microwave electromagnetic energy |
US4063151A (en) * | 1976-04-08 | 1977-12-13 | Schlumberger Technology Corporation | Microwave apparatus and method for determination of adsorbed fluid in subsurface formations surrounding a borehole |
US4077003A (en) * | 1976-04-08 | 1978-02-28 | Schlumberger Technology Corporation | Microwave method and apparatus utilizing dielectric loss factor measurements for determination of adsorbed fluid in subsurface formations surrounding a borehole |
US4107598A (en) * | 1976-02-02 | 1978-08-15 | Texaco Inc. | Electromagnetic wave logging system for determining resistivity and dielectric constant of earth formations |
US4278941A (en) * | 1978-10-30 | 1981-07-14 | Shell Oil Company | High frequency induction log for determining resistivity and dielectric constant of the earth |
US4360778A (en) * | 1978-10-30 | 1982-11-23 | Shell Oil Company | High frequency induction log for locating formation interfaces |
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4052662A (en) * | 1973-08-23 | 1977-10-04 | Schlumberger Technology Corporation | Method and apparatus for investigating earth formations utilizing microwave electromagnetic energy |
US4012689A (en) * | 1974-10-24 | 1977-03-15 | Texaco Inc. | Radio frequency resistivity and dielectric constant well logging utilizing phase shift measurement |
US4009434A (en) * | 1974-12-09 | 1977-02-22 | Texaco Inc. | Dielectric induction logging system for obtaining water and residual oil saturation of earth formations |
US4107598A (en) * | 1976-02-02 | 1978-08-15 | Texaco Inc. | Electromagnetic wave logging system for determining resistivity and dielectric constant of earth formations |
US4063151A (en) * | 1976-04-08 | 1977-12-13 | Schlumberger Technology Corporation | Microwave apparatus and method for determination of adsorbed fluid in subsurface formations surrounding a borehole |
US4077003A (en) * | 1976-04-08 | 1978-02-28 | Schlumberger Technology Corporation | Microwave method and apparatus utilizing dielectric loss factor measurements for determination of adsorbed fluid in subsurface formations surrounding a borehole |
US4151457A (en) * | 1976-04-08 | 1979-04-24 | Schlumberger Technology Corporation | Microwave method and apparatus for determination of adsorbed fluid in subsurface formations |
US4278941A (en) * | 1978-10-30 | 1981-07-14 | Shell Oil Company | High frequency induction log for determining resistivity and dielectric constant of the earth |
US4360778A (en) * | 1978-10-30 | 1982-11-23 | Shell Oil Company | High frequency induction log for locating formation interfaces |
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