CN106951666A - A kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field - Google Patents

A kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field Download PDF

Info

Publication number
CN106951666A
CN106951666A CN201710305146.0A CN201710305146A CN106951666A CN 106951666 A CN106951666 A CN 106951666A CN 201710305146 A CN201710305146 A CN 201710305146A CN 106951666 A CN106951666 A CN 106951666A
Authority
CN
China
Prior art keywords
temperature
annular space
fluid
drill string
node
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201710305146.0A
Other languages
Chinese (zh)
Other versions
CN106951666B (en
Inventor
孙万通
孟英峰
魏纳
周守为
李清平
李皋
郭平
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Southwest Petroleum University
Original Assignee
Southwest Petroleum University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Southwest Petroleum University filed Critical Southwest Petroleum University
Priority to CN201710305146.0A priority Critical patent/CN106951666B/en
Publication of CN106951666A publication Critical patent/CN106951666A/en
Application granted granted Critical
Publication of CN106951666B publication Critical patent/CN106951666B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2119/00Details relating to the type or aim of the analysis or the optimisation
    • G06F2119/08Thermal analysis or thermal optimisation

Abstract

The invention discloses a kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field, including:(1)Obtain ocean gas hydrate layer drilling parameter and primary condition;(2)Carry out space nodes division;(3)Set up ocean gas hydrate layer bored shaft calculation model for temperature field;(4)Fluid temperature (F.T.) in drill string at well head is the drilling fluid implantation temperature for calculating the momentT p(0) (n), the fluid temperature (F.T.) in annular space at well headT a(0) (n)The temperature of fluid is as returned out from annular space, it is assumed thatT a(0) (n)Value;(5)According to nodeiLocate fluid temperature (F.T.) in drill stringT p(i) (n)With fluid temperature (F.T.) in annular spaceT a(i) (n), calculate next nodeiThe temperature in wellbore at+1 place, obtains the fluid temperature (F.T.) at shaft bottom in drill stringT p(k) (n)With the fluid temperature (F.T.) in annular space at shaft bottomT a(k) (n);(6)Check whether to meet calculation error.The principle of the invention is reliable, is easy to operation, can be to judge ocean gas hydrate layer stable state, drilling fluid rheology, calculating Wellbore Flow parameter, and then ensures that marine drilling construction safety provides theoretical foundation.

Description

A kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field
Technical field
The invention belongs to marine drilling technical field, in particular it relates to ocean gas hydrate layer drilling technology method, Particularly a kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field.
Background technology
Gas hydrates are a kind of crystalline compounds being stable in the presence of under the conditions of low temperature, hyperbaric environment, its stock number Extremely enrich, in the bottom sediment for being mainly distributed on land permafrost band and continental margin periphery, wherein ocean natural gas is hydrated Thing stock number is about more than 100 times of land tundra.Ocean gas hydrate layer is under subsea cryogenic, hyperbaric environment, Keep relatively stable occurrence status.With the development of marine oil and gas drilling and production technology, marine drilling increases increasingly, and marine drilling is bored During entering, stratum, gas hydrates layer, stratum are drilled into successively, wherein, drilling fluid is at sea level from well head from drill string Inject pit shaft, flow through more than mud line well section i.e. residing for seawater, to mud line position be at seabed after, pass through i.e. stratum institute below mud line Locate well section, from drill bit flows out to annular space, then by returning to well head on annular space, pit shaft is returned out from annular space well head.
However, marine drilling is bored when meeting gas hydrates layer, because drill bit is in ocean gas hydrate layer, pit shaft The drilling fluid temperature of middle flowing is higher, can change the original temperature of ocean gas hydrate layer, and then influences hydrate Stable state, causes the decomposition gasification of hydrate, and wellbore construction is caused a significant threat safely.On the other hand, ocean natural gas In hydrate layer drilling well, it is different from the cutting grain in conventional marine drilling into the hydrate bore meal particles in mineshaft annulus, During it on annular space drilling fluid with returning, it can be reduced and decomposed due to temperature in wellbore rise, pressure, hydrate bore meal particles Decomposition heat-absorbing action can further influence temperature in wellbore change, therefore whole Wellbore Temperature Field can also can change, and then influence Drilling fluid rheology, Wellbore Flow Parameters variation.Therefore, the accurate meter in ocean gas hydrate layer bored shaft temperature field Calculate, to judging ocean gas hydrate layer stable state, drilling fluid rheology, calculating Wellbore Flow parameter, and then ensure sea Foreign wellbore construction has safely important directive significance.
At present, it is less to ocean gas hydrate layer bored shaft Study on Temperature Field both at home and abroad, the existing main pin of research To the Wellbore Temperature Field during marine drilling, when chance ocean gas hydrate layer is bored in research, hydrate is bored in annular space Bits particle is with returning the concurrent Wellbore Temperature Field estranged taken off on drilling fluid.Patent CN103226641A discloses a kind of deep water gas-liquid Two phase flow circulating temperature coupling pressure computational methods, pass through the order of annular space drilling fluid after drilling fluid in first drill string, iterative calculation Drilling fluid node temperature and pressure data in drill string and annular space, finally give deep-sea biphase gas and liquid flow temperature in wellbore and pressure simulation As a result, the method can apply the calculating of the Wellbore Temperature Field during marine drilling, but can not accurately reflect marine natural Wellbore Temperature Field during gas hydrate layer drilling well;Patent CN102943620A discloses a kind of based on drilling well annulus wellbore multiphase flow The dynamic controlled pressure drilling method calculated, during mineshaft annulus Multiphase Flow governing equation group is solved, required temperature in wellbore has embodied, But specific method for solving is not suggested that, it is impossible to be directly applied in ocean gas hydrate layer bored shaft Temperature calculating. Therefore, in the urgent need to a kind of Wellbore Temperature Field computational methods for ocean gas hydrate layer drilling well, ocean day is met when boring The influence that hydrate bore meal particles are decomposed in annular space is considered during right gas hydrate layer, it is stable to judge ocean gas hydrate layer State, drilling fluid rheology, calculating Wellbore Flow parameter provide theoretical foundation.
The content of the invention
It is an object of the invention to provide a kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field, the party Method principle is reliable, is easy to operation, can be to judge ocean gas hydrate layer stable state, drilling fluid rheology, calculate well Cylinder flow parameter, and then ensure that marine drilling construction safety provides theoretical foundation, with wide market prospects.
In order to realize above-mentioned technical purpose, the present invention uses following technical scheme.
Ocean gas hydrate layer drilling parameter and primary condition are obtained, space nodes division is carried out on this basis; Consider that gas hydrates bore meal particles decompose the influence of heat absorption, set up ocean gas hydrate layer bored shaft temperature field meter Model is calculated, obtains calculating the temperature change in grid;Then, according to the temperature at known node, the well at next node is calculated Cylinder temperature, according to the node in drill string and in annular space simultaneously from well head to the order in shaft bottom, iterates to calculate temperature in wellbore, until well Bottom temperature meets calculation error, then iteration terminates;Temperature in wellbore at all nodes of iterative calculation gained is ocean natural gas Hydrate layer bored shaft temperature field.
A kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field, comprises the following steps successively:
(1) according to Drilling Design and reservoir parameter, ocean gas hydrate layer drilling parameter and primary condition is obtained, is bored Well parameter includes:Casing programme, BHA, it is pumped into hydrate in parameter, sea water advanced, ocean temperature, formation temperature, reservoir Abundance, rate of penetration, well depth, primary condition include:Calculate the drilling fluid implantation temperature T at momentp(0) (n), annular space well head pressure pa(0) (n)
(2) space nodes division is carried out, according to ocean gas hydrate layer drilling parameter in step (1), spatial domain is Whole pit shaft, from well head to shaft bottom, node axial direction sequence number is incremented by successively since 0;During node ID at well head is 0, pit shaft Any calculate node sequence number represents that next calculate node sequence number is represented with i+1 with i, and node ID is k at shaft bottom.
(3) according to heat transfer theory and law of conservation of energy, ocean gas hydrate layer bored shaft temperature field is set up (Gao Yonghai, Sun Baojiang, Wang Zhi far wait deepwater drilling pit shaft temperature to temperature change expression formula in computation model, calculating grid as follows Spend calculating and analysis [J] the China University Of Petroleum Beijing's journals (natural science edition), 32 (2003) of field:58-62):
In drill string:
In annular space:
Mud line (at seabed) above well section, i.e. i Δs h < HseaWhen:
Mud line (at seabed) following well section, i.e. i Δs h >=HseaWhen:
In formula:I is calculate node;
N is the calculating moment;
Δ h is set as 1m to calculate Gridding length in calculating;
HseaFor sea water advanced, m;
ΔTp(i) (n)、ΔTa(i) (n)The temperature change in grid, K are calculated respectively in drill string, in annular space;
ρp(i)、ρa(i)Fluid-mixing density respectively in drill string, in annular space at calculate node i, kg/m3
vp(i)、va(i)Fluid-mixing flow velocity respectively in drill string, in annular space at calculate node i, m/s;
cp(i)、ca(i)Fluid-mixing specific heat capacity respectively in drill string, in annular space in pit shaft at calculate node i, J/ (kg K);
Dpi、Dpo、Dri、DciRespectively drill string internal diameter, drill string external diameter, water proof bore, casing inner diameter, m;
Qap(i)For heat exchange, W between fluid at calculate node i in annular space and drill string;
Qwa(i)、Qsa(i)Heat exchange, W between fluid at calculate node i respectively in seawater and annular space, in stratum and annular space;
Qfp(i)、Qfa(i)The heat produced respectively in drill string with flowage friction at calculate node i in annular space, W;
Qh(i)For the heat that decomposition of hydrate absorbs at calculate node i in annular space, W.
(4) when being i=0 at well head, the fluid temperature (F.T.) in drill string at well head is the drilling fluid implantation temperature for calculating the moment Tp(0) (n), it is known parameters according to the primary condition in step (1);And the fluid temperature (F.T.) T in annular space at well heada(0) (n)As from The temperature that fluid is returned out in annular space is unknown parameter, it is assumed that Ta(0) (n)Value, setting assume scope:273K≤Ta(0) (n)≤ Tp(0) (n)
(5) flowed according to the node in drill string and in annular space simultaneously from well head to the order in shaft bottom according in drill string at node i Temperature Tp(i) (n)With fluid temperature (F.T.) T in annular spacea(i) (n), calculate the temperature in wellbore at next node i+1:
In formula:Tp(i) (n)、Ta(i) (n)At respectively calculate node i in drill string, fluid temperature (F.T.), K in annular space;
Tp(i+1) (n)、Ta(i+1) (n)At respectively calculate node i+1 in drill string, fluid temperature (F.T.), K in annular space.
According to formula (4), (5), from well head iterative calculation until at the node k of shaft bottom, obtaining the fluid at shaft bottom in drill string Temperature Tp(k) (n)With the fluid temperature (F.T.) T in annular space at shaft bottoma(k) (n)
(6) iterated to calculate according to step (5) in obtained drill string, the fluid temperature (F.T.) in annular space at shaft bottom, it is fuller Sufficient calculation error:
In formula:Tp(k) (n)For the fluid temperature (F.T.) at shaft bottom in drill string, K;
Ta(k) (n)For the fluid temperature (F.T.) at shaft bottom in annular space, K;
γ is fluid temperature (F.T.) calculation error at shaft bottom, takes 1K.
If formula (6) is set up, calculation error is met, the drill string at all nodes as obtained by being iterated to calculate step (5) In, fluid temperature (F.T.) is ocean gas hydrate layer bored shaft temperature field in annular space.If formula (6) is invalid, no Calculation error is met, need to be to fluid temperature (F.T.) T at well head in the annular space in step (4)a(0) (n)Again it is assumed that simultaneously repeat step again (5) iterate to calculate, until formula (6) is set up.
In the step (3), heat exchange Q between fluid at calculate node i in annular space and drill stringap(i), count in seawater and annular space Heat exchange Q between fluid at operator node iwa(i), heat exchange Q between fluid at calculate node i in stratum and annular spacesa(i), calculate in drill string The heat Q that flowage friction is produced at node ifp(i), the heat Q that flowage friction is produced at calculate node i in annular spacefa(i) (Z.M.Wang,X.N.Hao,X.Q.Wang et al.Numerical simulation on deepwater drilling wellbore temperature and pressure distribution[J].Petroleum Science and Technology,28(2010):911-919) the heat Q that decomposition of hydrate absorbs at calculate node i and in annular spaceh(i) (E.D.Sloana,F.Fleyfelb.Hydrate dissociation enthalpy and guest size[J].Fluid Phase Equilibria,76(1992):Computational methods 123-140) are as follows:
Heat exchange Q between fluid at calculate node i in annular space and drill stringap(i)It is calculated as follows
Heat exchange Q in seawater and annular space at calculate node i between fluidwa(i)It is calculated as follows
Heat exchange Q in stratum and annular space at calculate node i between fluidsa(i)It is calculated as follows
Fluid and integrated heat transfer coefficient U of the stratum at calculate node i in annular space in formula (9)sa(i)It is calculated as follows
The heat Q that flowage friction is produced at calculate node i in drill stringfp(i)It is calculated as follows
The heat Q that flowage friction is produced at calculate node i in annular spacefa(i)It is calculated as follows
The heat Q that decomposition of hydrate absorbs at calculate node i in annular spaceh(i)It is calculated as follows
In formula (10)~(13):
Tw(i) (n)、Ts(i) (n)Ocean temperature, formation temperature, K at respectively calculate node i;
Dro、Dco、Dcso、DcsiRespectively marine riser external diameter, sleeve outer, cement sheath external diameter, cement sheath internal diameter, m;
αf1(i)、αf2(i)、αf3(i)Respectively drill string inner surface, water proof pipe internal surface, on internal surface of casing at calculate node i Forced convection heat transfer coefficient, W/ (m2·K);
αm1(i)、αm2(i)Respectively drill string outer surface, outer around face heat convection at calculate node i on water proof tube outer surface Coefficient, W/ (m2·K);
λp(i)、λr(i)、λc(i)、λcs(i)、λs(i)Respectively drill string, marine riser, sleeve pipe, cement sheath, stratum are in calculate node i The thermal conductivity factor at place, W/ (mK);
Usa(i)For fluid in annular space and integrated heat transfer coefficient of the stratum at calculate node i, W/ (m2·K);
TDFor Transient Heat Transfer function, zero dimension;
vp(i)、va(i)Flow velocity of the fluid-mixing at calculate node i, m/s respectively in drill string, in annular space;
mp(i)、ma(i)Mass flow of the fluid-mixing at calculate node i, kg/s respectively in drill string, in annular space;
DaoFor annular space external diameter, calculate node is water proof bore D positioned at mud line above well sectionri, positioned at mud line to go into the well Section is casing inner diameter Dci, m;
ZgeqFor the gas deviation factor under ring air temperature, pressure condition at node, zero dimension;
R is universal gas constant, J/ (molK);
peq(i) (n)For natural gas hydrate phase balance emulation pressure, Pa at calculate node i.
Compared with prior art, the present invention has following remarkable advantage:
(1) present invention according to the node in drill string and in annular space by, simultaneously from well head to the order in shaft bottom, iterating to calculate Wellbore Temperature Field is obtained, it is convenient to calculate, and error is smaller, accurately can quickly calculate Wellbore Temperature Field.
(2) present invention can realize its temperature in wellbore field computation for ocean gas hydrate layer drilling well, to judge sea Foreign gas hydrates layer stable state, drilling fluid rheology, calculating Wellbore Flow parameter, and then ensure marine drilling construction peace It is complete that theoretical foundation is provided.
Brief description of the drawings
Fig. 1 is ocean gas hydrate layer bored shaft heat exchange schematic diagram.
Fig. 2 is ocean gas hydrate layer bored shaft temperature field the actual calculation figure.
Embodiment
Below by taking the actual ocean gas hydrate layer drilling well in somewhere as an example, with reference to accompanying drawing, further is made to the present invention Explain, but the invention is not limited in following examples.
Ocean gas hydrate layer bored shaft heat exchange schematic diagram as shown in figure 1, mud line above pit shaft outside be seawater, Mud line with outside well-sinking for stratum.Drilling fluid injects in well head from drill string, and occurring heat by fluid in drill string and annular space hands over Change.Reach shaft bottom after, drilling fluid carry gas hydrates bore meal particles from annular space on return, on the one hand, fluid in annular space Occurs heat exchange with fluid in drill string;On the other hand, fluid is sent out by sleeve pipe, cement sheath and stratum in the following well section annular space of mud line Heat is exchanged, and by marine riser and seawater heat exchange occurs for fluid in mud line above well section annular space;On return during, gas water Compound bore meal particles influence Wellbore Temperature Field as temperature in wellbore is raised, pressure is reduced and heat absorption of decomposing.
A kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field, comprises the following steps successively:
(1) according to Drilling Design and reservoir parameter, ocean gas hydrate layer drilling parameter and primary condition are obtained:Every Water pipe outer diameter Dro, sleeve outer DcoIt is 0.508m;Drill string outer diameter DpoFor 0.127m, bit diameter is 0.445m;Well depth H is 1600m, is pumped into drilling fluid displacement 30l/s, is pumped into drilling fluid density ρp(0)For 1030kg/m3;Sea water advanced HseaFor 1500m;Sea Face temperature is 298K;Formation temperature gradient is 3 DEG C/100m;Hydrate abundance is 70% in reservoir;Rate of penetration is 10m/h;Meter Calculate the drilling fluid implantation temperature T at momentp(0) (n)For 298K;Annular space well head pressure pa(0) (n)For 101300Pa.
(2) space nodes division is carried out, according to ocean gas hydrate layer drilling parameter in step (1), spatial domain is Whole pit shaft, from well head to shaft bottom, node axial direction sequence number is incremented by successively since 0;Node ID at well head is at 0, shaft bottom Node ID is 1600.
(3) according to heat transfer theory and law of conservation of energy, based on ocean gas hydrate layer bored shaft temperature field Computation model, calculates the temperature change in grid:Δ T in drill stringp(i) (n)With Δ T in annular spacea(i) (n)
(4) it is that at node 0, when being calculated, the fluid temperature (F.T.) in drill string at well head is the brill for calculating the moment at well head Well liquid implantation temperature Tp(0) (n)For 298K;And the fluid temperature (F.T.) T in annular space at well heada(0) (n)Fluid is as returned out from annular space Temperature is unknown parameter, carries out hypothesis Ta(0) (n)Value, according to assume scope:273K≤Ta(0) (n)≤Tp(0) (n)It is assumed to be 292K, And calculated.
(5) flowed according to the node in drill string and in annular space simultaneously from well head to the order in shaft bottom according in drill string at node i Temperature Tp(i) (n)With fluid temperature (F.T.) T in annular spacea(i) (n), calculate the temperature in wellbore at next node i+1:Fluid temperature (F.T.) in drill string Tp(i+1) (n)With fluid temperature (F.T.) T in annular spacea(i+1) (n);Iterated to calculate from well head to shaft bottom, obtain the fluid at shaft bottom in drill string Temperature Tp(k) (n)Fluid temperature (F.T.) T in=281.06K, annular space at shaft bottoma(k) (n)=281.41K.
(6) according to the fluid temperature (F.T.) T in temperature in wellbore computational methods, obtained drill string in step (5) at shaft bottomp(k) (n)、 Fluid temperature (F.T.) T in annular space at shaft bottoma(k) (n), and according to calculation error γ=1K, more whether meet calculation error:Then meet calculation error.
Therefore, the fluid temperature (F.T.) T in annular space at well heada(0) (n)During for 292K, by calculating, fluid temperature (F.T.) is met at shaft bottom Calculation error, as obtained by being iterated to calculate step (5) at all nodes in drill string, fluid temperature (F.T.) is ocean natural gas in annular space Hydrate layer bored shaft temperature field, (Fig. 2 is ocean gas hydrate layer bored shaft temperature field example meter as shown in Figure 2 Calculate result figure).

Claims (3)

1. a kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field, comprises the following steps successively:
(1) according to Drilling Design and reservoir parameter, ocean gas hydrate layer drilling parameter and primary condition, drilling well ginseng are obtained Number includes:Casing programme, BHA, to be pumped into hydrate in parameter, sea water advanced, ocean temperature, formation temperature, reservoir rich Degree, rate of penetration, well depth, primary condition include:Calculate the drilling fluid implantation temperature T at momentp(0) (n), annular space well head pressure pa(0) (n)
(2) carry out space nodes division, spatial domain be whole pit shaft, from well head to shaft bottom, node axial direction sequence number since 0 successively It is incremented by, node ID at well head is that any calculate node sequence number is represented with i in 0, pit shaft, next calculate node sequence number i+1 Represent, node ID is k at shaft bottom;
(3) ocean gas hydrate layer bored shaft calculation model for temperature field is set up, the temperature change expression in grid is calculated Formula is as follows:
In drill string:
ΔT p ( i ) ( n ) = - 4 ρ p ( i ) v p ( i ) c p ( i ) πD p i 2 · ( Q a p ( i ) + Q f p ( i ) )
In annular space:
Mud line above well section,
The following well section of mud line,
In formula:I is calculate node,
N is the calculating moment,
Δ h is set as 1m to calculate Gridding length in calculating,
HseaFor sea water advanced, m,
ΔTp(i) (n)、ΔTa(i) (n)Temperature change respectively in drill string, in annular space in calculating grid, K,
ρp(i)、ρa(i)Fluid-mixing density respectively in drill string, in annular space at calculate node i, kg/m3,
vp(i)、va(i)Fluid-mixing flow velocity respectively in drill string, in annular space at calculate node i, m/s,
cp(i)、ca(i)Fluid-mixing specific heat capacity respectively in drill string, in annular space in pit shaft at calculate node i, J/ (kgK),
Dpi、Dpo、Dri、DciRespectively drill string internal diameter, drill string external diameter, water proof bore, casing inner diameter, m,
Qap(i)For heat exchange between fluid at calculate node i in annular space and drill string, W,
Qwa(i)、Qsa(i)Heat exchange between fluid at calculate node i respectively in seawater and annular space, in stratum and annular space, W,
Qfp(i)、Qfa(i)The heat produced respectively in drill string with flowage friction at calculate node i in annular space, W,
Qh(i)For the heat that decomposition of hydrate absorbs at calculate node i in annular space, W;
(4) when being i=0 at well head, the fluid temperature (F.T.) in drill string at well head is the drilling fluid implantation temperature T for calculating the momentp(0) (n)For Fluid temperature (F.T.) T in known parameters, annular space at well heada(0) (n)The temperature that fluid is returned out from annular space is unknown parameter, it is assumed that Ta(0) (n)Value;
(5) according to the node in drill string and in annular space simultaneously from well head to the order in shaft bottom, according to fluid temperature in drill string at node i Spend Tp(i) (n)With fluid temperature (F.T.) T in annular spacea(i) (n), calculate the temperature in wellbore at next node i+1:
T p ( i + 1 ) ( n ) = T p ( i ) ( n ) + ΔT p ( i ) ( n )
T a ( i + 1 ) ( n ) = T a ( i ) ( n ) + ΔT a ( i ) ( n )
In formula:Tp(i) (n)、Ta(i) (n)At respectively calculate node i in drill string, fluid temperature (F.T.) in annular space, K,
Tp(i+1) (n)、Ta(i+1) (n)At respectively calculate node i+1 in drill string, fluid temperature (F.T.) in annular space, K,
From well head iterative calculation until at the node k of shaft bottom, obtaining the fluid temperature (F.T.) T at shaft bottom in drill stringp(k) (n)With shaft bottom in annular space The fluid temperature (F.T.) T at placea(k) (n)
(6) if meeting following formula:
| T p ( k ) ( n ) - T a ( k ) ( n ) | < &gamma;
In formula:Tp(k) (n)For the fluid temperature (F.T.) at shaft bottom in drill string, K,
Ta(k) (n)For the fluid temperature (F.T.) at shaft bottom in annular space, K,
γ is fluid temperature (F.T.) calculation error at shaft bottom,
Fluid temperature (F.T.) is that ocean natural gas is hydrated in drill string, in annular space at all nodes as obtained by being iterated to calculate step (5) Nitride layer bored shaft temperature field.
2. a kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field as claimed in claim 1, its feature exists In hypothesis T in the step (4)a(0) (n)Value, its assume scope be 273K≤Ta(0) (n)≤Tp(0) (n)
3. a kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field as claimed in claim 1, its feature exists In fluid temperature (F.T.) calculation error γ takes 1K at shaft bottom in the step (6).
CN201710305146.0A 2017-05-03 2017-05-03 Method for calculating temperature field of drilling shaft of marine natural gas hydrate layer Expired - Fee Related CN106951666B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710305146.0A CN106951666B (en) 2017-05-03 2017-05-03 Method for calculating temperature field of drilling shaft of marine natural gas hydrate layer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710305146.0A CN106951666B (en) 2017-05-03 2017-05-03 Method for calculating temperature field of drilling shaft of marine natural gas hydrate layer

Publications (2)

Publication Number Publication Date
CN106951666A true CN106951666A (en) 2017-07-14
CN106951666B CN106951666B (en) 2020-03-27

Family

ID=59477916

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710305146.0A Expired - Fee Related CN106951666B (en) 2017-05-03 2017-05-03 Method for calculating temperature field of drilling shaft of marine natural gas hydrate layer

Country Status (1)

Country Link
CN (1) CN106951666B (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110674572A (en) * 2019-09-18 2020-01-10 西南石油大学 Method for predicting natural gas hydrate generation area in seabed gas transmission pipeline
CN112347675A (en) * 2020-10-13 2021-02-09 中国石油大学(华东) Method for cooperatively regulating and controlling reservoir natural gas hydrate phase state by drilling fluid additive and temperature and pressure field
CN117113777A (en) * 2023-09-08 2023-11-24 武汉理工大学 Drill string vortex-induced vibration calculation method considering internal flow

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040190589A1 (en) * 2003-03-13 2004-09-30 Alexander Zazovsky Determination of virgin formation temperature
CN104155226A (en) * 2014-07-24 2014-11-19 重庆大学 Reservoir penetrating media heat-fluid-solid coupling multi-phase fluid fracturing-seepage experimental system
CN104234680A (en) * 2014-09-12 2014-12-24 哈尔滨工程大学 Rapid thermal activation exploitation method for natural gas hydrate
CN104895560A (en) * 2015-06-16 2015-09-09 中国海洋石油总公司 Method for predicting wellbore pressure and temperature field simulation as well as hydrate through deep-water test
CN105486805A (en) * 2015-11-24 2016-04-13 西南石油大学 Multifunctional testing system and method for natural gas hydrate
CN106383360A (en) * 2016-08-16 2017-02-08 广东石油化工学院 Seismic data based submarine sediment temperature-pressure field recognition method
CN106930749A (en) * 2017-05-03 2017-07-07 西南石油大学 Gas Hydrate In Sea Areas layer drilling well equivalent permeability computational methods based on step-down

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040190589A1 (en) * 2003-03-13 2004-09-30 Alexander Zazovsky Determination of virgin formation temperature
CN104155226A (en) * 2014-07-24 2014-11-19 重庆大学 Reservoir penetrating media heat-fluid-solid coupling multi-phase fluid fracturing-seepage experimental system
CN104234680A (en) * 2014-09-12 2014-12-24 哈尔滨工程大学 Rapid thermal activation exploitation method for natural gas hydrate
CN104895560A (en) * 2015-06-16 2015-09-09 中国海洋石油总公司 Method for predicting wellbore pressure and temperature field simulation as well as hydrate through deep-water test
CN105486805A (en) * 2015-11-24 2016-04-13 西南石油大学 Multifunctional testing system and method for natural gas hydrate
CN106383360A (en) * 2016-08-16 2017-02-08 广东石油化工学院 Seismic data based submarine sediment temperature-pressure field recognition method
CN106930749A (en) * 2017-05-03 2017-07-07 西南石油大学 Gas Hydrate In Sea Areas layer drilling well equivalent permeability computational methods based on step-down

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
付强 等: "深水钻井天然气水合物井筒多相流动模型及敏感性分析", 《中国海上油气》 *

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110674572A (en) * 2019-09-18 2020-01-10 西南石油大学 Method for predicting natural gas hydrate generation area in seabed gas transmission pipeline
CN110674572B (en) * 2019-09-18 2022-03-11 西南石油大学 Method for predicting natural gas hydrate generation area in seabed gas transmission pipeline
CN112347675A (en) * 2020-10-13 2021-02-09 中国石油大学(华东) Method for cooperatively regulating and controlling reservoir natural gas hydrate phase state by drilling fluid additive and temperature and pressure field
CN112347675B (en) * 2020-10-13 2022-08-19 中国石油大学(华东) Method for cooperatively regulating and controlling reservoir natural gas hydrate phase state by drilling fluid additive and temperature and pressure field
CN117113777A (en) * 2023-09-08 2023-11-24 武汉理工大学 Drill string vortex-induced vibration calculation method considering internal flow
CN117113777B (en) * 2023-09-08 2024-04-09 武汉理工大学 Drill string vortex-induced vibration calculation method considering internal flow

Also Published As

Publication number Publication date
CN106951666B (en) 2020-03-27

Similar Documents

Publication Publication Date Title
Gao et al. A wellbore/formation-coupled heat-transfer model in deepwater drilling and its application in the prediction of hydrate-reservoir dissociation
CN103226641B (en) Coupling calculation method of deepwater gas-liquid two-phase flow circulating temperature and pressure
CN106968667A (en) A kind of temperature field prediction method and device
CN109598099B (en) Double-tube SAGD long horizontal well uniform steam injection numerical simulation method considering oil reservoir and shaft coupling
CN104895560B (en) A kind of deep water test wellbore pressure, temperature field simulation and Hydrate Prediction method
CN112627733B (en) Method and equipment for optimizing hydraulic parameters of deepwater pressure-controlled drilling in real time
CN111814100B (en) Method for dynamically simulating circulating temperature change of marine subsea pump lifting drilling system without marine riser
Xiao et al. Research on wellbore temperature control and heat extraction methods while drilling in high-temperature wells
CN106951666A (en) A kind of ocean gas hydrate layer bored shaft Calculation Method of Temperature Field
CN102682195B (en) Semisubmersible platform transient state bored shaft temperature computation method
CN115408956B (en) Hydrate reservoir drilling Zhou Wuxing and mechanical parameter real-time acquisition method
CN104343416A (en) Deep water gas well test system and test method
CN107060731A (en) A kind of deepwater drilling casing setting depth modification method based on well kick surplus
CN105822264B (en) Gas hydrates layer bored shaft hydrate dynamic Decomposition method for detecting position
CN111222281A (en) Gas reservoir type gas storage injection-production string erosion failure risk determination method
Zhao et al. Wellbore temperature distribution during drilling of natural gas hydrate formation in South China sea
CN115293066B (en) Gas well temperature field calculation method considering stratum seepage heat transfer effect
Wan et al. A feasibility study of producing natural gas from subsea hydrates with horizontal snake wells
Abdelhafiz et al. Effect of drilling and wellbore geometry parameters on wellbore temperature profile: Implications for geothermal production.
CN108316895B (en) Method for obtaining real-time drilling hole expansion rate of sea natural gas hydrate layer
Shan et al. Development of an analytical model for predicting the fluid temperature profile in drilling gas hydrates reservoirs
Feng et al. The transient temperature prediction in the deepwater riserless well
CN111927394A (en) Circulating system and method for continuously cooling high-temperature drilling fluid underground
CN117113766A (en) Shaft-reservoir coupling temperature field simulation and hydrate generation risk prediction method
CN117113765A (en) Wellbore-reservoir coupling temperature field and pressure field simulation method and system

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20200327

Termination date: 20210503