OA17323A - Sand detection using magnetic resonance flow meter. - Google Patents

Abstract

A method, apparatus and computer-readable medium for estimating a mass of silicates in a fluid flowing in a member is disclosed. A magnetic field is induced in the fluid to align nuclei of the fluid along a direction of the magnetic field. A radio frequency signal is transmitted into the fluid from a transmitter to excite silicon nuclei present in the fluid. A signal is received from the silicon nuclei responsive to the transmitted radio frequency signal at a receiver. A processor estimates the mass of silicates in the fluid directly from the received signal.

Description

BACKGROUND OF THE DISCLOSURE

1. Field of the Disclosure

10001J The présent disclosure is related to detecting the presence of silicates în flowing fluids.

2. Description of the Related Art [0002] Production operations recover fluids such as gas and/or liquid hydrocarbons from an underground formation via a production tubular. Solid particles, such as sand (silicate) grains, are often carried in the recovered fluid through the production tubular. These sand grains can cause érosion of various components of the production tubular, such as a pump for pumping the fluid, a flow control valve located on the tubular and the tubular itself. The effects of sand érosion can be costly to a production operation. The présent disclosure provides a method and apparatus for estimating amount of silicates in a fluid flowing in a production tubular in order that preventative actions can be taken.

SUMMARY OFTHE DISCLOSURE [0003J In one aspect, the présent disclosure provides a method of estimating a mass of silicates in a fluid flowing in a member, including: inducing a magnetic field in the fluid to align nuclei of tlie fluid along a direction of the magnetic field; transmitting a radio frequency signal into the fluid from a transmitter to excite silicon nuclei présent în the fluid; receiving a signal from the silicon nuclei responsive to the transmitted radio frequency signal at a receiver; and using a processor to estimate the mass of silicates in the fluid directly from the received signal.

[0004] In another aspect, the présent disclosure provides an apparatus for estimating a mass of silicates in a fluid flowing in a member, including: a magnetic source configured to induce a magnetic field in the fluid to align nuclei of the fluid along a direction of the magnetic field; a transmitter configured to transmit a radio frequency signal into the fluid to excite silicon nuclei présent in the fluid; a receiver configured to receive a signal from the silicon nuclei responsive to the transmitted radio frequency signal; and a processor configured to estimate the mass of silicates in the fluid directly from the rcceived signal.

[0005] In another aspect, the présent disclosure provides a computer-readable medium accessible to a processor, the computer-readable medium comprising instructions that cnable the processor to perform a method that includes: activatîng a transmitter to transmit a radio frequency signal into a fluid flowing in a member to excite the silicon nuclei of the fluid, wherein the nuclei are aligned along a direction of a magnetic field; receiving a signal from the silicon nuclei responsive to the transmitted radio frequency signal; and estimating a mass of silicates in the fluid directly from the rcceived signal.

[0006] Examples of certain features of the apparatus and method dîsclosed herein are summarized rallier broadly in order that the detailed description thereof that follows may be better understood. There are, of course, additional features of the apparatus and method disclosed hereinafter that will form the subject of the daims.

BRIEF DESCRIPTION OFTHE DRAWINGS [0007] For detailed understanding of the présent disclosure, référencés should be made to the following detailed description, taken in conjunction with the accompanying drawings, in which like éléments hâve been given like numerals and wherein:

FIG. 1 is a schematic élévation view of an exemplary welîbore having a production string installed therein;

FIG. 2 shows an exemplary sand détection device suitable for use in the exemplary production system of FIG. 1;

FIG. 3 shows an exemplary chemical shift spectrum of a silicaie obtained using exemplary Si²⁹ NMR methods of the présent disdosure;

FIG. 4 shows a graph displaying chemical shift ranges for various compounds; and

FIG. 5 shows an exemplary flowehart for determining a mass of silicates in a production fluid in an exemplary embodiment of the présent disclosure.

DETAILED DESCRIPTION OFTHE DISCLOSURE [0008] The présent disclosure relates to apparatus and methods for controlling flow of formation fluids in a production tubular. The présent disdosure provides certain exemplary drawings to dcscribe certain embodiments of the apparatus and methods that are to be considered examplcs ofthe principes described herein and are not intended to limit the concepts and disdosure to the illustrated and described embodiments.

* [0009J FIG. 1 shows an exemplary production wellbore system 100 that includes a wellbore 110 drilled through an earth formation 112 and into a production zone or réservoir 114. The wellbore 110 is shown lined with a casing having a number of perforations 118 that penetratc and extend into the formations production zones 114 so that production fluids may flow from the production zones 114 into the wellbore 110. The wellbore 110 includes a production string (or production assembly) 120 that includes a tubing (also referred to as the tubular or base pipe) 122 that extends downwardly from a wellhead 124 at the surface 126 of the wellbore 110. The production string 120 defines an internai axial bore 128 along its length. An annulus 130 is defined between the production string 120 and the wellbore casing. The production string 120 is shown to include a vertical section but may also include a generally horizontal portion that extends along a deviated leg or section of the wellbore (not shown). A production device 134 is positioned at a selected location along the production string 120. The production device 134 may be îsolated within the wellbore 110 by a pair of packer devices 136. Although only one production device 134 is shown, a large number of such production devices may be arranged along the production string 120.

[0010] The production device 134 includes a downhole-adjustable flow control device 138 to govem one or more aspects of flow of one or more fluids from the production zones into the production string 120. The downhole-adjustable flow control device 138 may hâve a number of alternative structural features that provide sélective operation and controlled fluid flow therethrough. The production string may further include an electrical submersible pump 102 for pumping fluid from within the production string 120 to a surface location.

[0011] Subsurface formations typically contain sand along with oil and gas. Asand screen is located at the production device 134 to separate sand from formation fluids prior to the formation fluid entering the production string. Tÿpically, a certain amount of sand passes through the sand screen due to effectiveness of the sand screen and wear on the sand screen. Sand détection device 200 may be used to déterminé an amount of sand presented in production fluid flowing in the tubular 122 using the exemplary methods discussed below.

[0012] FIG. 2 shows a detailed view of the sand détection device 200 used in the exemplary production system 100 of FIG. 1. The sand détection apparatus includes an exemplary Nuclear Magnetic Résonance (NMR) device which, in one embodiment, is configured to détermine the presence of silicates, such as kyanite, andalusite, quartz, etc. In various embodiments, the NMR device can also be used to détermine various parameters of the fluid flowing in the tubular, such as flow velocity, phase volume, hydrocarbon »

composition, etc. The sand détection apparatus can be coupled to a section of the tubular at a surface location including al a wellhead location. Altematively, the sand détection apparatus can be coupled to a section of the tubular at a downliolc location.

[0013] The NMR device inciudes a magnetic source 202 generally exterior to a section of the tubular 122. In various embodiments, the magnetic source may bc a permanent magnet or an eleclromagnelic. The magnetic source provides a substantially homogenous magnetic field which dermes a sensitive région in the section of the tubular. The NMR device also inciudes a transmitter 204 and a receiver 206. The transmitter may be an induction coil electricaïly coupled to transmitter electronics 208. The receiver may be an induction coil electrically coupled to receiver electronics 210. In an alternats embodiment, the transmitter and the receiver may be single coil electrically coupled to electronic circuitry that opérâtes the single coil in both a transmitter mode and a receiver mode. The transmitter coil 204 is configured to provide one or more radio frequency signais, known as NMR excitation puises, into the fluid flowing in the sensitive région. The transmitter electronics is configured to provide a radio frequency signal to the transmitter coil 204. The transmitter coil 204 is configured to induce a magnetic field of the excitation puise into the sensitive région. The frequency of the radio frequency signal may be selected to be substantially at a nuclear résonance frequency of an atomic nucléus of the fluid. Production fluids typically include hydrocarbons, consisting primarily of carbon and hydrogen atoms. Therefore, hydrogen NMR (H* NMR) and carbon NMR (C¹³ NMR) are generally used. For the purposes of the présent disclosure, the frequency of the excitation puise may be the résonant frequency of silicon isotope Si²⁹ or at a frequency of about 8.4578 MHz per Testa of magnetic field applied to obtain Si²⁹ NMR measurements indicative of silicon compounds, including silicates and silanes, for example. In one aspect of the présent disclosure, the transmitter electronics 208 may be tunable over a range of frequencies, thereby enabling transmitting of excitation puises at radio frequencies suîtable for H¹ NMR and C¹³ NMR measurements as well as for Si²⁹ NMR measurements.

[0014] The receiver electronics 206 is configured to receive one or more signais from the receiver coil 206. The signais from the receiver coil 206 are due to the response of nuclei in the fluid to an excitation puise fluid provided by the transmitter coil 204. The receiver electronics 206 may be configured to receive signais at a frequency consistent with the responsivc frequencies of Si²⁹ or may be configured to be tunable over a range of frequencies, thereby enabling receiver coil 206 to receive signais for H¹ NMR and C¹³ NMR measurements in addition to the Si²⁹ NMR signais.

[0015] In an exemplary method, NMR measurements are obtained from fluid flowing through tubular 122. In the exemplary embodiment of FIG. 2, fluid flows from left to right to enter the sensitive région defined by the magnetic field. The fluid may addîtionally flow through a pre-polarization section prc-polarizatîon magnet (not shown) prior to entering the sensitive région defined by the magnetic field. The nuclei of various atoms and molécules in the fluid are subjected to the magnetic field and align lhemselves so thaï the nuclear moments of the nuclei are oriented along the direction of lhe magnetic field. A radio frequency (RF) signal, known as an excitation puise, is applied to lhe aligned nuclei to perturb the nuclei from their aligned position using transmitter 204. The direction of the excitation puise is typically substantially perpendicular to the direction of lhe magnetic field. The excitation puise may include any number of excitation puise sequences known in the art for NMR testing including a Carr-Piircell-Meiboom-Gill (CPMG) puise sequence, for example. Upon being perturbed from alignment with the magnetic field, the nuclei tend to realign with the magnetic field at a given relaxation rate. Meanwhile, (he nuclei precess about lhe direction of the magnetic field and thereby produce a radio frequency signal which is received at rcccîvcr 206.

[0016] The sand détection apparatus also includes a control unit 212 which includes a processor 214, one or more computer programs 216 that are accessible lo lhe processor 214 for executing instructions contained in such programs to perform the methods dîsclosed herein to determined a mass of silicates in the fluid, and a storage device 134, such as a solidstate memory, lape or hard dise for storing the determining mass and other data obtained at the processor 130. Control unit 212 typically opérâtes transmitter electronics 208 to activate excitation puises into the sensitive région of the fluid via transmitter 204 and receives signais from receiver electronics 210 induced at receiver 206. Control unit 212 may addîtionally store data to a memory device 218 or send data to a display 220. Addîtionally, the control unit may providc an instruction to perform an operation based on lhe determined mass of silicates. Exemplary operations may include shutting down flow of fluid in the production string, rcplacing a component of the production string, such os a sand screen, a pump, etc. In addition, the calculated amount of silicates can be used to estimate a life span of various components of the tubular, such os lhe pump and/or the sand screen. In one embodiment, the processor 214 compares a determined mass amount of silicates to a threshold value and selects lhe operation based on lhe comparison.

[0017] Typically, atomic nuclei thaï hâve a total nuclear magnetic moment equal lo zéro arc unrcsponsive lo NMR methods, while atomic nuclei that hâve a non-zero nuclear magnetic moment are responsive to the magnetic field and excitation puise. Sand partides arc composed of silicates or Silicon dioxide (S1O2) compounds. The most abundant fomi of silicon is Si²⁸ which has a magnetic moment of zéro. However, Si²⁹ is a naturally occurring isotope of Si that has an isotopic abundance ofabout 4.7% and a non-zero magnetic moment. Therefore, NMR methods can be used to detect the presence of Si²⁹. Isotopic abundance calculations can then be used estimate an amount of Si²⁸ and/or a total amount of silicon compounds in the fluid. Similar mass calculations can be performed for H* NMR and C¹³ NMR methods, using an isotopic abundance of about 99.9% for H* and about 1.1% for C¹³.

[0018] For NMR methods, an excitation puise will be transmitted at a frequency which is known to excite the atomic nucléus of such that the nuclei resonate Qt a natural résonant frequency known as the Larmour frequency. The frequency v required to resonate the nuclei may be determined using the équation:

Eq.(l) where γ is the gyromagnetic ratio of the nudeus and B is the strength of the magnetic field.

[0019] The frequency at which the nuclei resonate after having been excited by the RF puise signal is typically different from the frequency of the excitation puise. The shift in résonant frequency is a resuit, in part, of different bond types, such as single bond and double bond as well as the atomic components. Therefore, the change in résonant frequency can be used to détermine a spedes of the compound. Generally, a ratio of the frequency of the received signal to the frequency of the RF excitation puise is calculated. This ratio is known as chemical shift and is measured in parts per million (ppm) using the équation below:

L» — V δ = —----------xlO ppm Eq. (2) where δ is the chemical shift, is the frequency of the received signal and v_w/toiinn is the frequency of the excitation puise.

[0020] FIG. 3 shows an exemplary chemical shift spectrum of a silicate obtained using exemplary Si²⁹ NMR methods using an excitation frequency of about 8.4578 MHz per Testa of magnetic field appiied. The exemplary spectrum exhibits a broad peak extending from about 100 ppm to about 130 ppm. The area under the peak is indicative of the number of the Si²⁹ atoms présent. Therefore, the processor 2I4 of the control unit 212 may be configured to détermine this area to'obtain a mass amount of the silicates in the fluid by determining the area under the peak and multiplying by an appropriate correction for Si²⁹ isotope abundance.

[0021] FIG. 4 shows a graph displaying chemical shîft ranges for various compounds including various hydrocarbon compounds such as aromatics, alkanes, alkenes ns well as for various silicon compounds such as silicon halides, silicates, silanes and transition métal silyl. FIG. 4 also shows a range of chemical shifts for water and TMS (Tetramethyl Silate). TMS 406 can be used as a calibration for Si³⁹ NMR measurements. The chemical shift of the hydrocarbon compounds are typicalîy obtained using H* NMR and C¹³ NMR measurements. The chemical shift of the silicon compounds may be obtained using Si²⁹ NMR measurements as described herein. Of the silicon compounds, silicon halides and transition métal silyls are typicalîy man-made compounds and therefore are typicalîy not seen in NMR measurements of production fluids obtained from a downhole formation. However, silicates 402 and silanes 404 are generally carried from downhole réservoirs and their spectrum typicalîy appears in NMR measurements of production fluids.

[0022] As stated with référencé to FIG. 3, the amount of a compound is related to the area under a spectrum représentative of the compound. In one embodiment, a mass of silicates in the fluid can be determined using Si²⁹ NMR methods. Si²⁹ NMR can be used to obtain a chemical shift spectrum from the fluid. The area of the spectrum from about -60 ppm to about -110 ppm can be calculated to estimate a mass of silicate material having the Si²⁹ isotope. The total silicate mass is then determined using the isotopic abundance of ratio of4.7% for Si²⁹.

[0023] If silicates are the only silicon compounds in the fluid, lhen the above method gives the total mass of silicates in the fluid. However, silanes are typicalîy also présent in production fluid and as seen in FIG. 4, the spectra for silicates and silanes overlap. Thus, a Si²⁹ NMR spectrum obtained from a production fluid will typicalîy hâve spectral contributions from both silicates and silanes. The Si²⁹ NMR spectrum may therefore yield a total mass of silicates and silanes, rather than a mass of silicates alone. In order to détermine the mass of the silicates, a mass of silanes may be determined and the determined silane mass is subtracted from the total mass of silicates and silanes.

[0024] Methods for determining the mass of silanes in the fluid are now discussed. Silanes include a single bond between silicon an hydrogen (-Si-H). Since silanes include both Si and H atoms, they are responsive to both Si²⁹ NMR and H* NMR. Since silicates include silicon and oxygen, they are generally unresponsîve to H¹ NMR. Therefore, a chemical shîft spectrum obtained using H¹ NMR from about +2 ppm to about -120 ppm mostly represents silanes. However, tt is apparent from FIG. 4, that the chemical shîft spectrum for silanes (from about 2 ppm to about -120 ppm) overlaps with the chemical shîft spectrum for alkanes (from about 1.5 ppm to about 0.8 ppm). Since both silanes and alkanes are responsive to H¹ NMR, the silane mass may be determined by determining the alkane mass separately and subtracting the alkane mass from a mass value (of silanes and alkanes) obtained from an H¹ NMR spectrum. C¹³ NMR may be used to obtain a mass of alkenes. The area under lhe C¹³ NMR spectrum from about 0.8 ppm to about 1.5 ppm yield a mass of alkanes having C¹³ isotopes. Multiplying this mass by a conversion factor using 1.1% C¹³ isotope abundance yields a total alkane mass in the fluid. It is noted that if the spectrum obtained from total H¹ NMR spectrum does not hâve contributions in lhe range at which alkane spectrum appears, there is no need to detect alkanes and therefore no need to use C¹³ NMR methods. Therefore, a method of determining silane mass is discussed below with respect to FIG. 5.

[0025] FIG. 5 shows an exemplary flowehart 500 for determining a mass of silicates in a fluid flowing in a member, such as a production fluid. In Box 502, a first mass is determined from a Si²⁹ NMR spectrum obtained from the fluid. The first mass represents the total mass of silanes and silicates in the fluid. The Si 29 NMR spectrum is obtained and a filter may be applied to the Si NMR spectrum to remove any contributions outside of the spectral range from about 2 ppm to about -120 ppm. A mass of silicon compounds having Si²⁹ is determined by calculai!ng an area under the fîltered Si²⁹ NMR spectral curve. The first mass may be obtained from the mass of Si²⁹ silicon compounds and an isotopîc abundance of Si²⁹ of 4.7%. In Box 504, a second mass is obtained using H* NMR. The second mass represents a mass of silanes and alkanes in the fluid. A spectrum is obtained using H¹ NMR. A filter is applied to the H¹ NMR spectrum to remove contributions outside of the spectral range from about 2 ppm to about -120 ppm. An isotopîc mass of H¹ is determined by calculating an area under the fîltered H¹ NMR spectral curve. H* isotopîc abundance is about 99.9% so either the isotopîc mass can bc multiplicd by the appropriate isotopîc abundance calculations or the isotopîc mass value can be taken as the total mass. In Box 506, a third mass is obtained using a C¹³ NMR. The third mass represents a mass of alkanes in lhe flutd. A spectrum is obtained using C¹³ NMR. A filter is applied to the C¹³ NMR spectrum to remove contributions outside of the spectral range from about 1.5 ppm to about 0.8 ppm. An isotopic mass for alkanes is determined by calculating an are under the fîltered C¹³ NMR spectral curve. The third mass is calculated using the obtained C¹³ mass and a 1.1% isotopic abundance of C¹³. In Box 508, lhe third mass (alkane mass) is subtracted from the second mass (total alkane and silanc mass) lo obtain a fourth mass (silane mass). In Box 510, tlie fourth mass (silanc mass) is subtrncted from the first mass (total silane and silicate mass) to obtain the total mass of silicates (sand). In équation form, lhe mass calculations is as follows:

Silkuin ⁼ Mgp — (m _fl( — MçU ) Eq. (3) [0026] Therefore, in one aspect, the présent disclosure provides a method of estimating a mass of silicates in a fluid flowing in a member, inciuding: inducing a magnetic field in the fluid to align nuclei of the fluid along a direction of the magnetic field; transmitlîng a radio frequency signal into lhe fluid from a transmitter to excite silicon nuclei présent în lhe fluid; receiving a signal from lhe silicon nuclei responsive to the transmitted radio frequency signal at a recetver, and using a processor to estimate the mass of silicates in the fluid directly from the receîved signal. The method may further include performing an operation based on the estimated mass of silicates that is one of: (i) shutting down the flow of fluid through the member, and (îi) estimating a life span of a component of the member. In an embodiment in which the fluid flows in the member via a sand screen, the method may include replacïng the sand screen at lhe member based on the estimated mass of silicates. In an embodiment in which the member includes a pump for pumping the fluid în the member, further comprising replacïng the pump based on the estimated mass of silicates. The method may include determining an isotopic mass of a compound from an NMR spectrum obtained from the fluid, and mulliplying lhe determined isotopic mass by an appropriate isotopic abundance ratio to détermine the total mass of the compound in the fluid. In one embodiment, the silicate mass îs détermine by: (i) determining a first mass from a Si²⁹ NMR spectrum obtained from the fluid; (ii) determining a second mass from an H* NMR spectrum obtained from the fluid; (iii) determining a third mass from a C¹³ NMR spectrum obtained from the fluid; <iv) subtracting the third mass from the second mass to obtain a fourth mass; and (v) subtracting the fourth mass from the first mass to obtain the mass of silicates in the fluid. The transmitted radio frequency signal may be transmitted from a tunable transmitter. The responsive signal may be rcceived at a tunable receiver. The magnetic field may be induced in the fluid at one of: (i) a surface location; (ii) a downhole location; and (iii) a wellhead.

[0027] In another aspect, the présent disclosure provides an apparatus for estimating a mass of silicates in a fluid flowing in a member, inciuding: a magnetic source configured to induce a magnetic field în lhe fluid to align nuclei of the fluid along a direction of the magnetic field; a transmitter configured to transmit a radio frequency signal into the fluid to ίο excite silicon nuclei présent in the fluid; a receiver configured to receive a signal from the silicon nuclei responsive to the transmitted radio frequency signal; and a processor configured to cstimate lhe mass of silicates in tire fluid dîrectly from the received signal. The processor may be further configured to perform an operation based on the estimated mass of silicates that is one of: (i) shutting down the flow of fluid in lhe member; and (ii) estimating a life span of a component of the tubular. For fluid flowing in the member via a sand screen, the processor may be further configured to provide an instruction to replace a sand screen at the member based on the estimated mass of silicates. For the member including a pump for pumping the fluid in the member, the processor may be further configured to provide an instruction to replace the pump based on the estimated mass of silicates. The processor may be configured to détermine an mass of an isotopic compound from an NMR spectrum obtained from the fluid, and multiply the estimated isotopic mass by an appropriate isotopic abundance ratio to obtain a total mass of the compound. In one embodiment, the processor is configured to: (i) détermine a first mass from a Si²⁹ NMR spectrum obtained from the fluid; (ii) détermine a second mass from a H* NMR spectrum obtained from the fluid; (iii) détermine a third mass from C¹³ NMR spectrum obtained from the fluid; (iv) subtract lhe third mass from the second mass to obtain a fourth mass; and (v) subtract the further mass from the first mass to obtain lhe mass of silanes présent in the fluid. In various embodiments, at least one ofthe transmitter and the receiver is tunable. The magnetic source is generally configured to induce the magnetic field at one of: (i) a surface location; (ii) a downhole location; and (iii) a wellhead.

[0028] ln another aspect, the présent disclosure provides a computer-readable medium accessible to a processor, lhe computer-readable medium comprising instructions that enable the processor to perform a method that includes: activating a transmitter to transmit a radio frequency signal into a fluid flowing in a member to excite the silicon nuclei of the fluid, wherein the nuclei are aligned along a direction of a magnetic field; receiving a signal from the silicon nuclei responsive to the transmitted radio frequency signal; and estimating a mass of silicates in the fluid dîrectly from the received signal. The computerreadable medium may further includes instructions to: obtain a first mass from a Si²⁹ NMR spectrum received at the processor from the fluid; obtain a second mass from a H¹ NMR spectrum received at the processor from lhe fluid; obtain a third mass from a C¹³ NMR spectrum received at the processor from lhe fluid; subtract the third mass from the second mass to obtain a fourth mass; and subtract the further mass from the first mass to estimate tlie mass of silicates in the fluid. Further instructions may include instructions to shut down flow n

of the fluid and/or cstimate a life time of a component of the member based on the estimated mass of silicates in the fluid. In one embodiment the medium includes instructions to détermine a mass of an isotopic compound in the fluid from an NMR spectrum obtained from the fluid and multiply the determined isotopic mass by an appropriate isotopic abundance ratio to obtain a total mass of the compound in the fluid.

(00291 While the foregoing disclosure is directed to the preferred embodiments of the disclosure, various modifications will be apparent to those skilled in the art. It is tntended that ail variations within the scope and spirit of the appended claims be embraced by the foregoing disclosure.

Claims (20)

1. A method of estimating a mass of si 1 icates in a fluid flowing in a member, comprising:

inducing a magnetic field in the fluid to align nuclei of the fluid along a direction of the magnetic field;

transmitting a radio frequency signal into the fluid from a transmitter to excite silicon nuclei présent in the fluid;

receiving a signal from the silicon nuclei responsive to the transmitted radio frequency signal at a receiver; and estimating the mass of silicates in lhe fluid directly from the received signal using a processor.

2. The method of claim 1 further comprising performing an operation based on the estimated mass of silicates, wherein the operation is at least one of: (i) shutting down the flow of fluid through lhe member, (ii) estimating a life span of a component of the member.

3. The method of daim 1, wherein the fluid flows in the member via a sand screen, further comprising replacing the sand screen at the member based on the estimated mass of silicates.

4. The method of daim 1, wherein the member comprises a pump for pumping the fluid in the member further comprising replacing the pump based on the estimated mass of silicates.

5. The method of claim 1 further comprising determining a mass of an isotopic compound in the fluid from an NMR spectrum obtained from the fluid, and multiplying the determined isotopic mass by an appropriate isotopic abundance ratio.

6. The method of claim 1 further comprising:

(i) determining a first mass from a Si²⁹ NMR spectrum obtained from the fluid;

(ii) determining a second mass from an H¹ NMR spectrum obtained from lhe fluid; and (iii) determining a third mass from a C¹³ NMR spectrum obtained from the fluid;

(iv) subtracting lhe third mass from the second mass to obtain a fourth mass; and (v) subtracting the fourth mass from the first mass to obtain lhe mass of silicates in the fluid.

7. The method of claim 1 further comprising at least one of: (i) transmitting the radio frequency signal from a tunable transmitter; and (ii) receiving the responsive signal at a tunable receiver.

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8. The method of claim 1 further comprising inducing the magnetic field in the fluid at one of: (î) a surface location; (ii) a downhole location; and (iii) a wellhead.

9. An apparatus for estîmating a mass of silicates in a fluid flowing tn a member, comprising:

a magnetic source configured to induce a magnetic field in the fluid to align nuclei of the fluid along a direction of lhe magnetic field;

a transmitter configured to transmit a radio frequency signal into the fluid to excite silicon nuclei présent in the fluid;

a receiver configured to receive a signal from the silicon nuclei responsive to the transmitted radio frequency signal; and a processor configured to estimate the mass of silicates in the fluid directly from the received signal.

10. The apparatus of claim 9, wherein the processor is further configured to perform an operation based on the estimated mass of silicates, wherein lhe operation is selected from the group consisting of: (i) shutting down the flow of fluid in lhe member; and (ii) estimatîng a life span of a component of the member.

11. Tlie apparatus of claim 9, wherein the fluid flows in the member via a sand screen, the processor further configured to provide an instruction to replace a sand screen at the member based on the estimated mass of silicates.

12. The apparatus of claim 9, wherein the member comprises a pump for pumping the fluid in the member, the processor further configured to provide an instruction lo replace the pump based on the estimated mass of silicates.

13. The apparatus of claim 9, wherein the processor is further configured to détermine a mass of an isotopic compound from an NMR spectrum obtained from the fluid, and multiply the determined isotopic mass by an appropriate isotopic abundance ratio.

14. The apparatus of claim 9, wherein lhe processor is further configured lo:

(i) détermine a first mass from a Si²⁹ NMR spectrum obtained from the fluid;

(ii) détermine a second mass from a H* NMR spectrum obtained from lhe fluid;

(iii) détermine a third mass from C¹³ NMR spectrum obtained from the fluid;

(iv) subtract the third mass from the second mass to obtain a fourth mass; and (v) subtract the further mass from the first mass to obtain the mass of silanes présent in the fluid.

15. The apparatus of claim 9, wherein at least one of: (i) the transmitter is a tunable transmitter; and (ii) the receiver is a tunable receiver.

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16. The apparatus of daim 9, wherein the magnetic source is further configured to induce the magnetic field at one of: (i) a surface location; (ii) a downhole location; and (îii) a wcllhead.

17. A computer-readable medium accessible to a processor, lhe computer-readable medium comprising instructions that enable the processor to perform a method that comprises:

activating a transmitter to transmit a radio frequcncy signal into n fluid flowing in a member to excite lhe silicon nudei of the fluid, wherein lhe nuclei are aligned along a direction of a magnetic field; and receive a signal from the silicon nudei responsîve to the transmitted radio frequcncy signa); and estimate a mass of silicates in the fluid directly from the received signal.

18. The computer-readable medium of claim 17 further comprising instructions to: obtain a first mass from a Si²⁹ NMR spectrum received at the processor from lhe fluid;

obtain a second mass from a H¹ NMR spectrum received at lhe processor from the fluid;

obtain a third mass from a C¹³ NMR spectrum received at the processor from the fluid.

subtract the third mass from the second mass to obtain a fourth mass; and subtract the further mass from the first mass to estimate the mass of silicates in the fluid.

19. The computer-readable medium of daim 17, wherein further comprising instructions to shut down flow of the fluid and estimate a life time of a component of the member based on the estimated mass of silicates in lhe fluid..

20. The computer-readable medium of claim 17, further comprising instructions to détermine a mass of an isotopic compound in the fluid from an NMR spectrum obtained from the fluid and multiply the determined isotopic mass by an appropriate isotopic abundance ratio.