3. kicks and gas migration.ppt
TRANSCRIPT
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PETE 625Well Control
Lesson 3
Kicks and Gas Migration
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Assignments
Homework #2:
Ch 1, Problems 1.11-1.21
Read: All of Chapter 1
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Density of Real Gases
M = molecular
weight
m = mass
n = no. of moles
gg= S.G. of gas
ZRT
pVn
V
nM
V
mg
29
M
M
M
ZRT
pM
V
M
ZRT
pV
air
g
g
ZRT
pgg
g29
(Real Gas Law)
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Density of Real Gases
What is the density of a 0.6 gravity gas at
10,000 psig and 200oF?
From Lesson 2, Fig. 1
ppr= p/ppc= 10,015/671 = 14.93
Tpr= (200+460)/358 = 1.84
Z = 1.413
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1.413
14.93
1.84
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Density of Real Gases
g= 2.33 ppg
TRZ
p29 gg
g
p = 10,000 psig
T = 200oF
gg= 0.6
{660)28.80(413.1
015,10)6.0(29g
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Equivalent Mud Weight,
EMW
The pressure, p (psig) in a wellbore, at
a depth of x(ft) can always beexpressed in terms of an equivalent
mud density or weight.
EMW = p / (0.052 * x) in ppg
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EMW
EMW is the density of themud that, in a column ofheight, x(ft) will generate the
pressure, p (psig) at thebottom, if the pressure at top= 0 psig
or, at TD:
p = 0.052 * EMW * TVD
0po=0
TVDp
x
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10
0
2,000
4,000
6,000
8,000
10,000
12,000
0.0 10.0 20.0 30.0 40.0 50.0
EMW, ppg
Dep
th,
ft
Depth
pEMW
*052.0
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0
2,000
4,000
6,000
8,000
10,000
12,000
0 1,000 2,000 3,000 4,000 5,000 6,000 7,000 8,000
Annulus Pressure, psig
Depth,
ft After Kick
Before Kick
SICP = 500 psig
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Gas Migration
Gas generally has a much lower density than
the drilling mud in the well, causing the gas to
rise when the well is shut in.
Since the gas, cannot expand in a closed
wellbore, it will maintain its pressure as it
rises (ignoring temp, fluid loss to formation,
compressibility of gas, mud, and formation)This causes pressures everywhere in the
wellbore to increase.
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13p1 = p2 = p3 ??
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Gas Migration
Example 1.7:A 0.7 gravity gas bubble
enters the bottom of a 9,000 ft vertical
well when the drill collars are being
pulled through the rotary table.
Flow is noted and the well is shut in with
an initial recorded casing pressure of 50
psig. Influx height is 350 ft.
Mud weight = 9.6 ppg.
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Gas Migration
Assume surface temperature of 70 oF.Temp gradient = 1.1
oF/100 ft. Surface
pressure = 14 psia
Determine the final casing pressure ifthe gas bubble is allowed to reach the
surface without expanding
Determine the pressure and equivalent
density at total depth under these final
conditions
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Gas Properties at Bottom
First assumption:BHP is brought to the surface
Pressure at the top of the bubble
P8,650= 14 + 50 + 0.052 * 9.6 * (9,000-350)
= 4,378 psia
T9,000= 70 + (1.1/100) * 9,000 + 460
= 629oR
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Gas Properties at Bottom
ppc= 666 psia
Tpc= 389 deg R
ppr= 4,378/666 = 6.57
Tpr= 629/389 = 1.62
Z = 0.925
pseudocritical - pseudoreduced
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Bottomhole Pressure
g= 29*0.7*4,378 / (0.925 * 80.28 * 629)
= 1.90 ppg
DpKICK= 0.052 * 1.9 * 350 = 35 psi
BHP = 4,378 + 35
BHP = 4,413 psia (~surface press.?
ZRTpg
gg29
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Pressure at Surface
Assume, at first, that Zf= 1.0 (at the surface)
Then,
46070*nR*0.1Vp
629*nR*925.0V378,4
ZnRTpV o
so, po= 3,988 psia (with Temp. corr.)
46070*0.1
p
629*925.0
378,4 o
BOTTOM SURFACE
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Solution with Z-factor
A few more iterative steps result in
Z0= 0.705 and p0= 2,812 psia
At the surface
f= 29*0.7*2,812 / (0.705*80.28*530)
= 1.9 ppg
ZRT
pgg
g29
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New BHP & EMW
New BHP = 2,812 + 0.052 * 1.9 * 350+ 0.052 * 9.6 * 8,650
New BHP = 7,165 psia
EMW = (7,165 - 14)/(0.052 * 9,000)
EMW = 15.3 ppg
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1. 4,413 psia2. 4,378
3. 3,988 (T)
4. 3,258 (Z)
5. 2,812 (Z)
6. 2,024 (mud)
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Compression of Mud in Annulus
vA = 0.1 bbl/ft)DV = compressibility * volume * Dp
= -6 * 10-6(1/psi) * 0.1(9,000-350)*2,626
DV = -13.63 bbls
Initial kick volume = 0.1 * 350 = 35 bbls
New kick volume = 35 + 13.63
= 48.63 bbl
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Compression of Mud in Annulus
From Boyles Law, pV = const
p2* 48.63 = 2,812 * 35
p2= 2,024 psiap8650 poA poB poC
Consider: V,p,Z const. p,Z change mud comp.
2nd iteration ? . 3rd
or, Is there a better way?
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Gas Migration Rate
A well is shut in after taking a 30 bbl
kick. The SIDPP appears to stabilize at
1,000 psig. One hour later the pressure
is 2,000 psig.
Ann Cap = 0.1 bbl/ft
MW = 14 ppg
TVD = 10,000 ft
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Gas Migration Rate
How fast is the kick migrating?
What assumptions do we need to make
to analyze this question?
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1 hr
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First Attempt
If the kick rises x ft. in 1 hr and the
pressure in the kick = constant, then
the pressure increases everywhere,
Dp = 0.052 * 14 * x
x = (2,000 - 1,000) / (0.052 * 14)
x = 1,374 ft
Rise velocity = 1,374 ft/hr
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Gas Migration Rate
Field rule of thumb ~ 1,000 ft/hr
Laboratory studies ~ 2,0006,000 ft/hr
Who is right?
Field results?
Is the previous calculation correct?
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Second Attempt
Consider mud compressibility
Ann. capacity = 0.1 bbl/ft * 10,000 ft
= 1,000 bbl of mud
Volume change due to compressibility
and increase in pressure of 1,000 psi,
DV = 6*10-6(1/psi) * 1,000 psi * 1,000 bbl
= 6 bbl
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Second Attempt
i.e. gas could expand by 6 bbl, to 36 bbl
Initial kick pressure=1,000 + 0.052 * 14 * 10,000 (approx.)
= 8,280 psig
= 8,295 psia
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Second Attempt
A 20% expansion would reduce the
pressure in the kick to ~ 0.8*8,295
= 6,636 psia
= 6,621 psig
So, the kick must have migrated morethan 1,374 ft!
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Second Attempt
How far did it migrate in 1 hour?
The pressure reduction in kick fluid
= 8,260 - 6,621=1,659 psi
The kick must therefore have risen an
additional x2ft, given by:
1,659 = 0.052 * 14 * x2
x2= 2,279 ft
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Second Attempt
2nd estimate = 1,374 + 2,279
= 3,653 ft/hr
What if the kick size is only 12 bbl?
What about balooning of the wellbore?
What about fluid loss to permeable
formations? T? Z?...
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Example 1.9
Kick occurs. After shut-in, initial csg.
Press = 500 psig. 30 minutes later,
p = 800 psig
What is the slip velocity if the kick
volume remains constant?
MW = 10.0 ppg
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Simple Solution
hrttftpsi
g
psippv
12
12slip
Ignoring
temperature,
compressibility and
other effects.
5.00.10052.0
500800vslip
hr/ft154,1vslip
What factors affect
gas slip velocity, or
migration rate?
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Gas slip velocity
The bubble size, and the size of the
gas void fraction, will influence
bubble slip velocity.
The void fraction is defined as the
ratio (or percentage) of the gas
cross-sectional area to the total flowarea.
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Gas slip velocity
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Gas slip velocity
Bubbles with a voidfraction > 25%
assume a bullet nose
shape and migrate
upwards along the
high side of the
wellbore concurrent
with liquid backflow,on the opposite side of
the wellbore
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Gas slip velocity
Large bubbles rise faster than smallbubbles
Other factors:
Density differencesHole geometry
Mud viscosity
Circulation rateHole inclination
One lab study showed max. rate at 45o.