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2900 - Site Mitigation Program
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PR0543397
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Last modified
2/10/2020 11:21:23 AM
Creation date
2/10/2020 9:37:25 AM
Metadata
Fields
Template:
EHD - Public
ProgramCode
2900 - Site Mitigation Program
File Section
COMPLIANCE INFO
RECORD_ID
PR0543397
PE
2965
FACILITY_ID
FA0012215
FACILITY_NAME
RCCI PTP
STREET_NUMBER
14253
Direction
S
STREET_NAME
AIRPORT
STREET_TYPE
WAY
City
MANTECA
Zip
95336
APN
19803031
CURRENT_STATUS
01
SITE_LOCATION
14253 S AIRPORT WAY
P_LOCATION
04
P_DISTRICT
003
QC Status
Approved
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EHD - Public
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SPE 16798 PRAMOD K. SINGH, RAM G. AGARWAL AND LOREN D. KRASE 7 <br /> straight line drawn through steps after wellbore 4. Data influenced by wellbore storage and <br /> fillup has an intercept much above the pretest p.-es- changing wellbore storage will plot with a con- <br /> sure point (pref 1060 psi at zero rate) suggesting cave upward curvature on the p vs. q plot. It <br /> that these steps are above the parting pressure. is incorrect to force a straight line through <br /> This is confirmed by the Odeh and Jones multirate these steps. <br /> analysis plot shown in Fig. 24. FPP is therefore <br /> interpreted to be 2169 psi, the pressure at the end 5. Multirate analysis can be applied to determine <br /> of the third step. the parting pressure provided the time step <br /> size is at least long enough to be in a <br /> 2. Field Example B storage-radial transition flow regime. Accu- <br /> rate kh analysis, however, requires the data to <br /> This illustrates the use of linear flow multi- be in a purely radial flow regime. <br /> rate analysis to determine parting pressure for a <br /> fractured well. The well was shut-in for a falloff 6. The rate-time history before a SRT and the <br /> test just before the SRT. Analysis of the falloff pressure at the start of the SRT should be <br /> data indicated a uniform flux fracture of 110 ft recorded for valid multirate analysis. The <br /> half-length. The SRT consisted of 1-hour time steps proper application of multirate analysis has <br /> of approximately 500 bpd rate increments. been demonstrated. <br /> The p (surface pressures, corrected for frit- 7. Linear flow superposition is a powerful tool <br /> tional pressure loss) vs. q plot is shown in for determining parting pressure from SRT data <br /> Fig. 25. Data for the early steps form a concave on a fractured well. Shorter time steps, lim- <br /> upward curvature. This behavior may be observed ited to the duration of Linear flow, can be <br /> simply due to superposition effects even for steps used in this case. <br /> with linear flow. Based on the interpretation (two <br /> straight lines) shown in Fig. 25, parting pressure B. The techniques developed in this paper have <br /> would be interpreted to be between steps 13 and 14, been successfully applied to field SRT data. <br /> at 975 psi. <br /> NOMENCLATURE <br /> The radial flow Odeh and Jones plot for this <br /> case did not give a clear indication of parting b' = intercept of line from Odeh and Jones anal- <br /> pressure and is not shown. Fig. 26 is the linear ysis (see Eq. 3) <br /> flow Odeh and Jones plot. The falloff before the <br /> SRT is accounted for as a transient step and pres- B = formation volume factor, RB/STB (res m3/stock <br /> sure at the end of the falloff (p FF) is used for tank m3) <br /> superposition. Clearly, data for rtge first ten <br /> steps fall on a single curve. A shift in data for c = total system compressibility, psi 1 (kPa 1) <br /> steps beyond step 10 indicates that these steps are <br /> above the parting pressure. The true FPP is there- C = wellbore storage factor, RB/psi (res m3/kPa) <br /> fore interpreted to be 744 psi, the pressure at the <br /> end of the tenth step. FCD = dimensionless fracture conductivity <br /> Note that for this example the p vs. q plot h = formation thickness, ft (m) <br /> (Fig. 25) does not show a definite change in slope <br /> corresponding to the FPP. In fact, data points for k = formation permeability, and <br /> all the steps form a smooth S-shaped curve. <br /> Interpretation for parting pressure from this plot m' = slope of line from Odeh and Jones analysis <br /> is, therefore, very subjective. Clearly, linear (see Eq. 2) <br /> flow multirate analysis is a superior analysis tool <br /> for this case. p = pressure, psi (kPa) <br /> CONCLUDING REMARKS Pref = pressure at the beginning of a rate change <br /> (beginning of the SRT, see Fig. 14), psi <br /> A systematic investigation of a number of sig- (kPa) <br /> nificant factors affecting SRT design and analysis <br /> has been made. Based on the results of this inves- Ap = pressure change, psi (kPa) <br /> tigation, the following conclusions can be made: <br /> q = flow rate, negativefor injection, STB/D or <br /> 1. Previously available guidelines for SRT proce- Mscf/D ("standard" m3/D) <br /> dure and analysis are not adequate. <br /> q = long term stabilized rate prior to the SRT <br /> 2. Equal size time steps of length long enough to L (see Fig. 14), STB/D or Mscf/D ("standard" <br /> be out of wellbore storage should be used for m3/D) <br /> an ideal SRT. <br /> q = reduced or changed rate prior to the SRT (see <br /> 3. Data completely dominated by wellbore storage r Fig. 14), STB/D or Mscf/D ("standard" m3/D) <br /> will plot with a unit slope on a log-log plot <br /> of dp vs. cumulative injection (production) for r = radius, ft (m) <br /> a constant wellbore storage factor. <br /> s = skin factor <br /> 497 <br />
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