Vogel problems often involve flow efficiency (FE). Why? They both need Pwf & Pr.
Example: Say Pwf = 1M and Pr = 2M psi at q = 490 BOPD. What is qmax?
Go to the Vogel table (7 PRD 1) with Pwf/Pr = 0.5; note qo/qmax = 0.7.
So qmax = qo/0.7 = 490/0.7 = 700
BOPD.
But what then if FE is 0.7 and we stimulate to an FE = 1? See 12 WLT 2:
Another way to describe FE: the percentage of well fluid producing at a given drawdown compared to what it would produce with zero skin (FE = 1).
So at FE = 1.7M/0.7 = 1,000 BOPD.
Thursday, June 28, 2018
Wednesday, June 27, 2018
Hydrostatic: 2005 #24 (similar)
Sand at 9,000 ft. Pr = 4,000 psi. Two fluids. Which A-B-C option below is 500 psi underbalanced?
(A) 3,000 ft 0.1 ppf N2 cushion, 6,000 ft 10 ppg, 80-psi surface pressure.
(B) 2,000 ft 0.1 ppf N2 cushion, 7,000 10 ppg, 160-psi surface pressure.
(C) 2,500 ft 0.1 ppf N2 cushion, 6,500 10 ppf, 400-psi surface pressure.
Use the hydrostatic pressure equation (2 DRL 1). Calculating pressures p = 0.052(D)MW) + gradient(D) + surface pressure - reservoir pressure for:
(A) 300 + 3,120 + 80 - 4,000 = -500 psi
(B) 200 + 3,640 + 160 - 4,000 = 0 psi
(C) 250 + 3,380 + 400 - 4,000 = 30 psi
Expect this sort of problem with any fluid, depths, or pressures. Just remember to line them up in an orderly fashion; speed is of the essence.
(A) 3,000 ft 0.1 ppf N2 cushion, 6,000 ft 10 ppg, 80-psi surface pressure.
(B) 2,000 ft 0.1 ppf N2 cushion, 7,000 10 ppg, 160-psi surface pressure.
(C) 2,500 ft 0.1 ppf N2 cushion, 6,500 10 ppf, 400-psi surface pressure.
Use the hydrostatic pressure equation (2 DRL 1). Calculating pressures p = 0.052(D)MW) + gradient(D) + surface pressure - reservoir pressure for:
(A) 300 + 3,120 + 80 - 4,000 = -500 psi
(B) 200 + 3,640 + 160 - 4,000 = 0 psi
(C) 250 + 3,380 + 400 - 4,000 = 30 psi
Expect this sort of problem with any fluid, depths, or pressures. Just remember to line them up in an orderly fashion; speed is of the essence.
Tuesday, June 26, 2018
Net Piston Force: 2005 #23 (similar)
Here the "Net Piston Effect" is shown.
Say Csg & Tbg pressure changes are:
dPcp = 500 psi (often given as pre-post job csg pressure).
dPtp = 3,000 psi (often calculated by hydrostatic).
Packer, Tbg, & Csg areas: Apb, Ati, Ato = 7.1, 7.0, 9.2 sq in (given or from dia).
The packer (7.1) is larger than tbg id (7); so the GB predicts a negative (up) force:
Fp = dPCp(Apb-Ato) - dPTp(Apb - Ati)
Fp = 500(7.1-9.2)-3,000(7.1 - 7.0) = -1,385 lbf (up).
Fp = 500(-2.1) - 3,000(0.1)
Fp = -1,050-300 = -1,385
Fp = 500(7.1-7) - 3,000(7.1-9.2) = -1,385 lbf (up). This checks.
To calculate tbg length change? Say the tubing is 10,000'; tbg area is 9.2 - 7 = 1.8 sq in:
LtF/EAt = (10,000 ft*1,385 lbf)/(30M*1.8) = 0.15'*12 = -1.8 inches (up)
The entire tubing move section is a single page, with all the variables listed to the right.
Monday, June 25, 2018
Balloon Force: 2005 #22 (similar)
6 DTC 9 is one of my favorite Guidebook pages (TBG Move). It shows all the forces you will need on a single page. It was a labor of love.
So if you are asked for the force from say the ballooning effect, it's just a glance: Keep in mind the dPt and dPc are pressure changes, so find the initial and final pressures in both the casing and the tubing.
You typically chase down the BHTP using hydrostatic. For example at 10,000 ft, 8 ppg:
Initial Tubing: 0.052(8)10,000 = 4,160 psi. If surface: 0 psi, dPTa1 = 2,100 psi
Final Tubing: Surface & BHP say 6,000 & 7,900 psi you average: dPTa2 = 6,950 psi
From initial & final tubing psi, find the change by subtracting: 6,950 - 2,100 = 4,850 psi
Casing pressure change is often just given as an increase, say 1,000 psi.
Calculate or look up the tubing ID & OD area. That's easy; here we will use 7.0 & 9.6 in.
Thus: -0.6 [(4850*7) - (1000*9.6)] = -14,600 psi (up).
The units are negative (note the sign in front) which means tension.
Since pressure increased, we should indeed see tension if the packer is fixed.
These problems can be very confusing. Go slow; be sure the numbers make sense. Once you've done a few, it's fairly easy.
So if you are asked for the force from say the ballooning effect, it's just a glance: Keep in mind the dPt and dPc are pressure changes, so find the initial and final pressures in both the casing and the tubing.
You typically chase down the BHTP using hydrostatic. For example at 10,000 ft, 8 ppg:
Initial Tubing: 0.052(8)10,000 = 4,160 psi. If surface: 0 psi, dPTa1 = 2,100 psi
Final Tubing: Surface & BHP say 6,000 & 7,900 psi you average: dPTa2 = 6,950 psi
From initial & final tubing psi, find the change by subtracting: 6,950 - 2,100 = 4,850 psi
Casing pressure change is often just given as an increase, say 1,000 psi.
Calculate or look up the tubing ID & OD area. That's easy; here we will use 7.0 & 9.6 in.
Thus: -0.6 [(4850*7) - (1000*9.6)] = -14,600 psi (up).
The units are negative (note the sign in front) which means tension.
Since pressure increased, we should indeed see tension if the packer is fixed.
These problems can be very confusing. Go slow; be sure the numbers make sense. Once you've done a few, it's fairly easy.
Sunday, June 24, 2018
Beam Counterbalance: 2005 #20 (similar)
Counterbalance is calculated fairly easily. No fancy charts; it's all in the Guidebook.
Rod Pump equations are found on a single page 7 PRD 9.
The counterbalance equation (CBE) is step #27. It references steps #1, #5, #15-16. Again, easy:
#1: Wr is found on 7 PRD 10 in C3, and is the Wgt Rods / ft in air (lbf/ft)
#5: Fo = 0.340(G)D^2(H) which is Fluid Weight On Pump (lbf)
#15: W = Wr∙L which is Weight Rods total in air (lbf)
#16: Wrf = W(1−0.128 G) which is the Weight Rods total in fluid (lbf)
#27: CBE = 1.06(Wrf + 0.5 Fo)
The GB makes this calculation simple plug-and-chug. Just march through the steps.
Here, I'll assume standard 76 rods, 1.5 plunger, & SG = 0.85 (get this from oil API as needed).
#1: Wr = 1.833 (7 PRD 10 column 3 for 76 rods)
#2: Fo = 0.34(0.85)1.5^2(8,800') = 5,850 lb
#15: W = 1.833 lb/ft(8,800') = 16,500 lb
#16: Wrf = 16,500 lb [1-(0.128*0.85)] = 14,700 lb
#27: CBE 1.06 (14,350 + 0.5*5720) = 18,700 lb.
In real life, you may measure CB to find the difference between calculated CBE and actual CB.
For example, if measured CB was 18,500 lb, you are 200 lb short.
Be careful on these problems to keep it simple. Don't panic at all the possible options from extra data like dyno cards, unit type, etc. Just assume it's going to be simple, focus, and march through the steps.
Every item on this type of problem can be found in the GB: Wr, Fo, W, CBE. It's in tables on 7 PRD 9, in order, with a typical number.
Rod Pump equations are found on a single page 7 PRD 9.
The counterbalance equation (CBE) is step #27. It references steps #1, #5, #15-16. Again, easy:
#1: Wr is found on 7 PRD 10 in C3, and is the Wgt Rods / ft in air (lbf/ft)
#5: Fo = 0.340(G)D^2(H) which is Fluid Weight On Pump (lbf)
#15: W = Wr∙L which is Weight Rods total in air (lbf)
#16: Wrf = W(1−0.128 G) which is the Weight Rods total in fluid (lbf)
#27: CBE = 1.06(Wrf + 0.5 Fo)
The GB makes this calculation simple plug-and-chug. Just march through the steps.
Here, I'll assume standard 76 rods, 1.5 plunger, & SG = 0.85 (get this from oil API as needed).
#1: Wr = 1.833 (7 PRD 10 column 3 for 76 rods)
#2: Fo = 0.34(0.85)1.5^2(8,800') = 5,850 lb
#15: W = 1.833 lb/ft(8,800') = 16,500 lb
#16: Wrf = 16,500 lb [1-(0.128*0.85)] = 14,700 lb
#27: CBE 1.06 (14,350 + 0.5*5720) = 18,700 lb.
In real life, you may measure CB to find the difference between calculated CBE and actual CB.
For example, if measured CB was 18,500 lb, you are 200 lb short.
Be careful on these problems to keep it simple. Don't panic at all the possible options from extra data like dyno cards, unit type, etc. Just assume it's going to be simple, focus, and march through the steps.
Every item on this type of problem can be found in the GB: Wr, Fo, W, CBE. It's in tables on 7 PRD 9, in order, with a typical number.
Saturday, June 23, 2018
Rod Pump Volumetric Efficiency: 2005 #17 (similar)
Volumetric Efficiency for a rod pump is an easy problem. So do it fast.
7 PRD 9 is the Guidebook page for all Rod Pump equations. It's got everything; no flipping pages! For a quick example from the page:
1) Pump volume displaced equation: PD = 0.1166(Sp)D^2(N).
2) Total fluid pumped is usually given: say 370 BFPD.
3) Given pump data: Sp = 90"*, D = 2", N = 10 SPM.
*Sp, or stroke, is often presented as the pump third number (see 7 PRD 9).
Calculation: 0.1166(90)2^2(10) = 420 BPD
Volumetric Efficiency = BFPD/PD = 380/420 = 90%
7 PRD 9 is the Guidebook page for all Rod Pump equations. It's got everything; no flipping pages! For a quick example from the page:
1) Pump volume displaced equation: PD = 0.1166(Sp)D^2(N).
2) Total fluid pumped is usually given: say 370 BFPD.
3) Given pump data: Sp = 90"*, D = 2", N = 10 SPM.
*Sp, or stroke, is often presented as the pump third number (see 7 PRD 9).
Calculation: 0.1166(90)2^2(10) = 420 BPD
Volumetric Efficiency = BFPD/PD = 380/420 = 90%
Rod Pump: 2005 #18 (similar)
Q: What pumping unit change reduces torque the least? 1) Reducing stroke length or speed, 2) Changing rotation direction, or 3) Installing larger rods?
A: Reducing stroke length or speed lowers torque. Larger rods? This doesn't "reduce" torque at all. So that would be my choice.
On a sidenote: changing direction is a bit more tricky to consider. Why? Class III (& Mark II) API specs recommend the crank arm rotate in the counterclockwise direction only. Class I can operate in either direction but this is not recommended for many reasons. Greater torque spikes clockwise is one of them.
Friday, June 22, 2018
PBU: 2005 #16 & #68 (similar)
The standard pressure buildup (PBU) question wants skin, pressure drop, or radius of investigation (ROI). 12 WLT 12:
Variables:
B FVF bbl/STB
ct compressibility 1/psi
h thickness reservoir ft
k permeability md
MTR middle time region
p pressure psia
pwf pressure well flow psia
q flow rate well last STB/hr
ri radius investigation ft
rw radius wellbore ft
tp time produced pre-SI hr
Δt time new well SI after tp hr
ϕ porosity x.xx
μ viscosity cp
Example: q = 100 BO/D, h = 50 ft, Bo = 1.4 RB/STB, μ = 0.8 cp, & a graph of psi vs (tp-Δt)/Δt with an MTR of m = 300 psi (use one log cycle):
k = [162.6(100 BO/D)1.4 rb/STB(0.8 cp)]/[300*50 ft] = 2.25 md
From here, the ROI from SI pressure transient (say after 2 days) calculates from a simple equation on 12 WLT 6. A few more variables like ϕ (say 12%) and ct (say 4E-6 /psi) are needed:
ri = [2.25 md(48 hr)]/[948(0.12)(0.8 cp)4.3E-6 psi]^0.5 = 540 ft
Skin is calculated using tp (say 72 hr) and PBU data (tp+Δt)/Δt. Use Δt = 1 hr (easier division); this means (tp+Δt)/Δt = (72 hr+1 hr)/1 hr = 73 hrs. Now: back-extrapolate MTR to 73 hrs for pressure; 2,500 psi is a typical value. Subtract from given Pwf for drawdown (say 1,000 psi) and then divide by slope m over one log cycle.This is the skin equation's first term. 6.5 would be typical.
Using our our prior data, plus the well diameter (assume 4 in diameter) we can calculate skin:
s = 1.151[(P1hr-Pfbhp)/m]-log[k/[(por)(vis)ct(rw^2)]+3.23
= 1.151[6.5-log[2.25[(0.12*0.8*4.3E-6*0.125^2]+3.23
= 1.151[6.5-6.7+3.23] = 3.5
Variables:
B FVF bbl/STB
ct compressibility 1/psi
h thickness reservoir ft
k permeability md
MTR middle time region
p pressure psia
pwf pressure well flow psia
q flow rate well last STB/hr
ri radius investigation ft
rw radius wellbore ft
tp time produced pre-SI hr
Δt time new well SI after tp hr
ϕ porosity x.xx
μ viscosity cp
Example: q = 100 BO/D, h = 50 ft, Bo = 1.4 RB/STB, μ = 0.8 cp, & a graph of psi vs (tp-Δt)/Δt with an MTR of m = 300 psi (use one log cycle):
k = [162.6(100 BO/D)1.4 rb/STB(0.8 cp)]/[300*50 ft] = 2.25 md
From here, the ROI from SI pressure transient (say after 2 days) calculates from a simple equation on 12 WLT 6. A few more variables like ϕ (say 12%) and ct (say 4E-6 /psi) are needed:
ri = [2.25 md(48 hr)]/[948(0.12)(0.8 cp)4.3E-6 psi]^0.5 = 540 ft
Skin is calculated using tp (say 72 hr) and PBU data (tp+Δt)/Δt. Use Δt = 1 hr (easier division); this means (tp+Δt)/Δt = (72 hr+1 hr)/1 hr = 73 hrs. Now: back-extrapolate MTR to 73 hrs for pressure; 2,500 psi is a typical value. Subtract from given Pwf for drawdown (say 1,000 psi) and then divide by slope m over one log cycle.This is the skin equation's first term. 6.5 would be typical.
Using our our prior data, plus the well diameter (assume 4 in diameter) we can calculate skin:
s = 1.151[(P1hr-Pfbhp)/m]-log[k/[(por)(vis)ct(rw^2)]+3.23
= 1.151[6.5-log[2.25[(0.12*0.8*4.3E-6*0.125^2]+3.23
= 1.151[6.5-6.7+3.23] = 3.5
Wednesday, June 20, 2018
Archie Cementation Factor m: 2005 #11 (similar)
Given a formation with known porosity (say 9%), Ro (say 25 ohmm), and Rw from a core test (say 0.25 ohmm): calculate the formation cementation factor (or exponent m; this may be called either).
Two equations for F are on 15 LOG 1, with 2 variables each. Given 3 of the variables (we are missing only m) this is easy to solve. The Guidebook actually gives the equation for m here so it's just plug-and-chug.
Problems like this may show many sample points; if so, it doesn't matter which you choose. But you can check your work using a second set if you have the time.
F = Ro/Rw = 25/.25 = 100
F = 1/por^m = 1/0.09^m
(m)log(por) = log(1/F)
m = log(1/F)/log(por)
m = log(1/100)/log(.09)
m = -2/-1.05 = 1.9
Be aware on other problems you may be asked for (or given) a tortuosity factor "a" (F=a/por^m) rather than a = 1 (the norm). It's all on the 15 LOG 1 page if this unlikely event arises.
Two equations for F are on 15 LOG 1, with 2 variables each. Given 3 of the variables (we are missing only m) this is easy to solve. The Guidebook actually gives the equation for m here so it's just plug-and-chug.
Problems like this may show many sample points; if so, it doesn't matter which you choose. But you can check your work using a second set if you have the time.
F = Ro/Rw = 25/.25 = 100
F = 1/por^m = 1/0.09^m
(m)log(por) = log(1/F)
m = log(1/F)/log(por)
m = log(1/100)/log(.09)
m = -2/-1.05 = 1.9
Be aware on other problems you may be asked for (or given) a tortuosity factor "a" (F=a/por^m) rather than a = 1 (the norm). It's all on the 15 LOG 1 page if this unlikely event arises.
Tuesday, June 19, 2018
Mud Cleaning: 2005 #7 (similar)
One must often select the most cost effective mud cleaning equipment given a desired particle size. Those problems are easy using 4 MUD 6 of the Guidebook (below is the relevant part):
Solid Control Equipment Order:
1. Shale Shaker: down to 75 μm particle size
Mesh ex: 70x30: 70 openings/in one direction, 30 in perpendicular
Degasser (vacuum pump) or Gas Separator (no pump)
2. Mud tank:
Mud Agitator: prevents “steeling”
Mud Gun: flushes tanks
3. Desander: down to 45 μm, Desilter down to 15 μm
…fine screens can replace desander/desilter for power savings
Mud Cleaner: parts 1-3
4. Hydrocyclone: changes flow path; solids into cones
5. Centrifuge: rotating drum; rotation speed variable
6. Additives: Chemical, Bentonite, Water
75 + μm? Shaker.
75 - 45 μm? Shaker + Desander.
45 - 15 μm? Shaker + Desander + Desilter.
Solid Control Equipment Order:
1. Shale Shaker: down to 75 μm particle size
Mesh ex: 70x30: 70 openings/in one direction, 30 in perpendicular
Degasser (vacuum pump) or Gas Separator (no pump)
2. Mud tank:
Mud Agitator: prevents “steeling”
Mud Gun: flushes tanks
3. Desander: down to 45 μm, Desilter down to 15 μm
…fine screens can replace desander/desilter for power savings
Mud Cleaner: parts 1-3
4. Hydrocyclone: changes flow path; solids into cones
5. Centrifuge: rotating drum; rotation speed variable
6. Additives: Chemical, Bentonite, Water
75 + μm? Shaker.
75 - 45 μm? Shaker + Desander.
45 - 15 μm? Shaker + Desander + Desilter.
Sunday, June 17, 2018
Pump HP: 2005 #3 (similar)
Calculating drilling pump horsepower? Total pressure drop is needed (pipe, bit, annulus, surface).
We will assume annulus & surface pressure drop is 0.
All 5 equations needed are on a single Guidebook page, 3 HYD 1.
1) For pipe pressure drop (say MW=10ppg, PV=40cp, V=14 fps, 500 gpm, 10M ft):
dP/dL= (ρ0.75 V1.75 μ0.25)/1,800 d1.25
dPd/10,000 = (100.75 141.75 400.25)/1,800*3.81.25
dPd = 1,500 psi.
2) Not given pipe ID? Merely back-calculate ID from your 14 fps & 500 gpm:
d=[q/2.448V]^1/2 = 500/[2.448*14)] = 3.8 in.
3) For bit pressure loss (given nozzle area = 0.39 si):
dPb = 8.311E-5 MW q2/[CD2 At2] dPb = 8.311E-5(10)5002/[0.952 0.392d
Pb = 1,500 psi.
4) So total pressure drop over the pumping system is 1,500 + 1,500 = 3,000 psi.
5) Enter this into the standard HP equation:
[dP q]/1,714 = 3,000*500/1714 = 875 HP.
This is a tricky problem; step 2 is especially mean. Yet the equations do logically progress on a single Guidebook page, making it easier.
We will assume annulus & surface pressure drop is 0.
All 5 equations needed are on a single Guidebook page, 3 HYD 1.
1) For pipe pressure drop (say MW=10ppg, PV=40cp, V=14 fps, 500 gpm, 10M ft):
dP/dL= (ρ0.75 V1.75 μ0.25)/1,800 d1.25
dPd/10,000 = (100.75 141.75 400.25)/1,800*3.81.25
dPd = 1,500 psi.
2) Not given pipe ID? Merely back-calculate ID from your 14 fps & 500 gpm:
d=[q/2.448V]^1/2 = 500/[2.448*14)] = 3.8 in.
3) For bit pressure loss (given nozzle area = 0.39 si):
dPb = 8.311E-5 MW q2/[CD2 At2] dPb = 8.311E-5(10)5002/[0.952 0.392d
Pb = 1,500 psi.
4) So total pressure drop over the pumping system is 1,500 + 1,500 = 3,000 psi.
5) Enter this into the standard HP equation:
[dP q]/1,714 = 3,000*500/1714 = 875 HP.
This is a tricky problem; step 2 is especially mean. Yet the equations do logically progress on a single Guidebook page, making it easier.
Saturday, June 16, 2018
Collapse; Tension & Pressure: 2005 #2 (similar)
Given: 7 in. P-110 casing (D/t = 7/0.59) with axial tension of 50M & internal pressure of 11M psi. Collapse pressure (psi)?
Combined tension and pressure? Complex. Use 6 DTC 4:
1) (σz + pi)/σyield = (50M + 11M)/110M = 0.554
2) Chart: --> 0.544 ---> -0.60 = (pi - pcrr)/pcr (note negative sign for collapse)
3) pcrr = pi - (-0.60)pcr) = pi + 0.6(pcr) = 11M + 0.6(pcr)
We're here in less than 2 minutes but still need pcr. The Redbook shows 7 in. P-110 casing's collapse rating is 16,990 psi. Of course you can calculate it (from D & t; see the formula on 6 DTC 2) but it's faster to use the Redbook. This allows us to calculate collapse pressure in this situation:
pcrr = pi - (-0.60)pcr) = pi + 0.6(16,990) = 11M + 10.1M = 21.1M.
3 minutes. Not bad! We've lost at least half our engineers by now on an exam. Last but not least: do a quick mental check; does internal pressure strengthen or weaken collapse? Clearly strengthen, and that's what the equation shows. Just be careful; it's easy to make a sign mistake.
Combined tension and pressure? Complex. Use 6 DTC 4:
1) (σz + pi)/σyield = (50M + 11M)/110M = 0.554
2) Chart: --> 0.544 ---> -0.60 = (pi - pcrr)/pcr (note negative sign for collapse)
3) pcrr = pi - (-0.60)pcr) = pi + 0.6(pcr) = 11M + 0.6(pcr)
We're here in less than 2 minutes but still need pcr. The Redbook shows 7 in. P-110 casing's collapse rating is 16,990 psi. Of course you can calculate it (from D & t; see the formula on 6 DTC 2) but it's faster to use the Redbook. This allows us to calculate collapse pressure in this situation:
pcrr = pi - (-0.60)pcr) = pi + 0.6(16,990) = 11M + 10.1M = 21.1M.
3 minutes. Not bad! We've lost at least half our engineers by now on an exam. Last but not least: do a quick mental check; does internal pressure strengthen or weaken collapse? Clearly strengthen, and that's what the equation shows. Just be careful; it's easy to make a sign mistake.
Thursday, June 14, 2018
Petroleum PE Problems 2018: 1-40
The 2018 Guidebook Companion is available on Amazon. I only publish these on Kindle to keep the cost <$10.
The sample problems look great on a smartphone or computer using the free Kindle app. The format displays two problems per page; all you need is scratch paper.
These problems reference the 2018 Guidebook exclusively (which has new sections and additional material). It also leans heavy on the SPE Handbook (although every problem can be solved using the 2018 Guidebook alone).
These practice problems were reviewed by three different 2017 PE exam takers, each giving it the thumbs-up. Harder than the 2016 and 2017 versions in my opinion (with some new twists) so I think they offer a challenge to nearly everyone. However, I personally find the 2016 version the most applicable to reality, and many agree with me. YMMV. I've been surprised at the diversity of opinion out there: one person's yawn is another person's bane.
My intent is to have problems 41-80 out by September; wish me luck.
The sample problems look great on a smartphone or computer using the free Kindle app. The format displays two problems per page; all you need is scratch paper.
These problems reference the 2018 Guidebook exclusively (which has new sections and additional material). It also leans heavy on the SPE Handbook (although every problem can be solved using the 2018 Guidebook alone).
These practice problems were reviewed by three different 2017 PE exam takers, each giving it the thumbs-up. Harder than the 2016 and 2017 versions in my opinion (with some new twists) so I think they offer a challenge to nearly everyone. However, I personally find the 2016 version the most applicable to reality, and many agree with me. YMMV. I've been surprised at the diversity of opinion out there: one person's yawn is another person's bane.
My intent is to have problems 41-80 out by September; wish me luck.
Monday, June 11, 2018
ESP
Some interesting points regarding ESPs: the older SPE Handbook (Bradley 1987) has two seemingly contradictory quotes on the same page (7-1):
a) The ESP has the broadest producing range of any artificial lift method.
b) The major disadvantage of the ESP is that it has a narrow producing rate range compared with other artificial lift forms.
What is correct? Here's what the newer SPE Handbook says regarding ESPs:
1. 200 to 20M B/D typical (30M max).
2. High-Volume Lift Capacity excellent
3. Low-Volume Lift Capacity generally poor: low efficiency & high operation costs <400 BFPD.
4. Limited by needed horsepower.
5. Can be restricted by casing size.
Hard to know what Bradley was trying to say. Just be aware of both SPE sources, and let this be a lesson on how language can make an otherwise simple question more difficult. I like to underline these "money quotes" in pencil in my Handbook when I run across them.
Friday, June 8, 2018
SPE Petroleum Engineering Certification and PE License Exam Reference Guide (Ghalambor, 2014)
Below is my Amazon review. I'm posting this here since I get so many questions about this book. As you can see, I like the book, but not for the PE Exam. Why? It's designed for a different exam, lacks number examples for the equations, and is not easy to search to find the correct formula. Feel free to ask questions or make your own assessment in the comment section below.
To be clear about what this book is: it’s a list of equations, graphs, and tables. They are broken up into the following six subjects:
Reservoir Engineering
Drilling Engineering
Formation Evaluation
Production Engineering
Facilities
Petroleum Economics
Strong points:
1. Comprehensive. I would add a few here and there, but one must draw the line somewhere.
2. Clear print. Big graphs.
3. Each variable listed after the equation.
Weak points:
A. No numbers shown with equations! This makes many hard to use, even if you understand them.
B. No explanations! You better understand these equations before you use them.
C. Let’s be clear: this book is just a list of equations/graphs/tables, nothing more.
D. No easy way to find what you need besides the six chapters. You have to know this book well to make it useful on an exam.
E. Ring bound. This is both a plus and minus, just be aware of it.
In summary: if you want a comprehensive book of equations without numbers or examples, this book is for you. I’ve found it makes for a useful office reference. Just don’t expect much more except some graphs and tables (which are not comprehensive, but pretty complete for general use). It is the primary and only allowed reference for the Certification Exam, but I wouldn't bring it to the Professional Engineering Exam unless I knew it very well and supplemented it with notes.
To be clear about what this book is: it’s a list of equations, graphs, and tables. They are broken up into the following six subjects:
Reservoir Engineering
Drilling Engineering
Formation Evaluation
Production Engineering
Facilities
Petroleum Economics
Strong points:
1. Comprehensive. I would add a few here and there, but one must draw the line somewhere.
2. Clear print. Big graphs.
3. Each variable listed after the equation.
Weak points:
A. No numbers shown with equations! This makes many hard to use, even if you understand them.
B. No explanations! You better understand these equations before you use them.
C. Let’s be clear: this book is just a list of equations/graphs/tables, nothing more.
D. No easy way to find what you need besides the six chapters. You have to know this book well to make it useful on an exam.
E. Ring bound. This is both a plus and minus, just be aware of it.
In summary: if you want a comprehensive book of equations without numbers or examples, this book is for you. I’ve found it makes for a useful office reference. Just don’t expect much more except some graphs and tables (which are not comprehensive, but pretty complete for general use). It is the primary and only allowed reference for the Certification Exam, but I wouldn't bring it to the Professional Engineering Exam unless I knew it very well and supplemented it with notes.
Monday, June 4, 2018
SPE Petroleum Engineering Handbook (Bradley 1987)
There are only a few useful SPE books for the PE Exam. Bradley's SPE Petroleum Engineering Handbook is one. On the used market it goes for $100 to $200. My Amazon review is here.
I bring this up because I'm often returning to Bradley. I'm amazed at how concise and well-organized this text is. I'm currently updating my reservoir section with a few "money quotes" from Bradley. Remember, this is still an SPE reference, and thus it's fair game on the PE Exam.
In fact, I know several people who used it exclusively for their PE Exam and did well. One of the reasons it still shines for the exam is how tight it is: no wasted words. Clear explanations. Simple format for quick reference. And it has a lot of practical, work-related stuff the newer Handbook series leaves out for some reason.
In summary: because the new Handbook Series is out, people are selling their old Bradley Handbooks thus making them at least "somewhat" affordable. Back in the day, it was a collector's item and very hard to even find. So while quite dated it's worth another look as a primary reference.
I bring this up because I'm often returning to Bradley. I'm amazed at how concise and well-organized this text is. I'm currently updating my reservoir section with a few "money quotes" from Bradley. Remember, this is still an SPE reference, and thus it's fair game on the PE Exam.
In fact, I know several people who used it exclusively for their PE Exam and did well. One of the reasons it still shines for the exam is how tight it is: no wasted words. Clear explanations. Simple format for quick reference. And it has a lot of practical, work-related stuff the newer Handbook series leaves out for some reason.
In summary: because the new Handbook Series is out, people are selling their old Bradley Handbooks thus making them at least "somewhat" affordable. Back in the day, it was a collector's item and very hard to even find. So while quite dated it's worth another look as a primary reference.
Wednesday, May 30, 2018
Petroleum Engineering Guidebook 2018: Now Available
Over the last two years, the Petroleum Engineering Guidebook has had five printings. And some major improvements along the way.
The original book was merely my own unedited notes, albeit carefully compiled for a decade. I gave copies of these away to friends and other engineers taking the PE Exam.
However, as new requests overwhelmed my limited printing resources (and my wife's patience) I listed it on Amazon to cover printing costs. I then slowly cleaned up the typos over 2016 and 2017 (with suggestions from other engineers; thank you, you know who you are!). The latest edition, an officially bound, paperback book, is sold, printed, and shipped directly from Amazon.
The Guidebook was always intended for industry use. Because of this, I kept practice problems separate. Upon request, however, I generated digital problems that test-takers can use alongside the Guidebook for practice. Note I provide digital format only and advise not bringing practice problems to the PE Exam itself. Why? If you waste time trying to find the "right" type of problem you will likely do yourself more harm than good. Those test-writers are smarter than that.
So the most current book (2018, 1st edition) is a $55 paperback. It's got new additions requested by 2016 & 2017 test-takers (such as hydrates, economics, probability, decision trees, bits, produced water, etc.).
Here's the thing: if you have purchased a spiral copy from me through Amazon I'll replace it with the new paperback at cost. Just mail me your old book with a self-addressed, stamped envelope and PayPal my email $3 (or put it in envelope) to offset printing costs (but email me first so I can verify you are an original purchaser & get a book ready). It's going to be a first-come, first-serve thing.
UPDATE: I'm mailing off 3 books today but I still a lot left. So even those who have plagiarized versions (there are a lot floating around), send me an email and we can arrange a swap of some kind. The new version is much better, especially for the exam.
The original book was merely my own unedited notes, albeit carefully compiled for a decade. I gave copies of these away to friends and other engineers taking the PE Exam.
However, as new requests overwhelmed my limited printing resources (and my wife's patience) I listed it on Amazon to cover printing costs. I then slowly cleaned up the typos over 2016 and 2017 (with suggestions from other engineers; thank you, you know who you are!). The latest edition, an officially bound, paperback book, is sold, printed, and shipped directly from Amazon.
The Guidebook was always intended for industry use. Because of this, I kept practice problems separate. Upon request, however, I generated digital problems that test-takers can use alongside the Guidebook for practice. Note I provide digital format only and advise not bringing practice problems to the PE Exam itself. Why? If you waste time trying to find the "right" type of problem you will likely do yourself more harm than good. Those test-writers are smarter than that.
So the most current book (2018, 1st edition) is a $55 paperback. It's got new additions requested by 2016 & 2017 test-takers (such as hydrates, economics, probability, decision trees, bits, produced water, etc.).
Here's the thing: if you have purchased a spiral copy from me through Amazon I'll replace it with the new paperback at cost. Just mail me your old book with a self-addressed, stamped envelope and PayPal my email $3 (or put it in envelope) to offset printing costs (but email me first so I can verify you are an original purchaser & get a book ready). It's going to be a first-come, first-serve thing.
UPDATE: I'm mailing off 3 books today but I still a lot left. So even those who have plagiarized versions (there are a lot floating around), send me an email and we can arrange a swap of some kind. The new version is much better, especially for the exam.
Thursday, May 3, 2018
PEH Volume I Chapter 12: Crude Oil Emulsions
C1-3: Math
C4: Fluid Sampling
C5: Gas Properties
C6: Oil Correlations
C7: Thermo/Phase
C8: Phase Diagrams
C9: Asphaltene/Wax
C10: Produced Water
C11: Phase Behavior
C12: Emulsions
C13: Rock Properties
C14: Permeability
C15: Relative Permeability
C16: Economics
C17-18: Law
C4: Fluid Sampling
C5: Gas Properties
C6: Oil Correlations
C7: Thermo/Phase
C8: Phase Diagrams
C9: Asphaltene/Wax
C10: Produced Water
C11: Phase Behavior
C12: Emulsions
C13: Rock Properties
C14: Permeability
C15: Relative Permeability
C16: Economics
C17-18: Law
Emulsions are a common yet poorly-understood oilfield reality. Like hydrates, they seem to slip through the cracks and few want to claim them: do they belong to facilities, PVT, or production? I've just added yet another page to the Guidebook that deals with this complicated subject (7 PRD 13). The primary source? PEH chapter 12. See below:
Produced water:
normally “free”; if an emulsion, typically:
water droplets dispersed (as
internal phase, same surface area)…
…within oil or other (the
external/continuous phase).
May be: “water in oil” (up to 80% water cut), or “oil in
water” (>80% water cut), or more complex.
Emulsions:
found everywhere; reservoir, wellbore,
wellhead, facility, plant.
Created by:
mixing (valves, pores, etc.) + emulsifier (stabilizing agent,
such as fine solids & surfactants).
Surfactants: compounds
partly soluble in oil and water.
Water-wet particles stabilize oil-in-water
emulsions; Oil-wet particles stabilize water-in-oil emulsions.
Natural emulsions
come from the “heavy” crude fraction.
Asphaltenes change wettability of solids so they act
as emulsifiers.
Waxes crystalize if cooled below “cloud point” and
create emulsions.
Tighter emulsions mean more, smaller droplets
(more stable).
Sedimentation: settling water in an emulsion (due
to oil/water density differences).
Creaming: raising oil droplets in the water phase
(due to higher density of oil).
Emulsion treatment
(demulsify) typically means removing water & associated salts.
Demulsification
breaks emulsion to oil & water phases: 2 steps 1) flocculation, 2) coalescence.
Flocculation: aggregation/agglomeration/coagulation
of component phases.
Coalescence: droplets irreversibly
fuse (larger drops/lower surface area); high water cut enhanced.
Treatments: chemical
(common), heating (common), electrostatic field (coalescence),
settling.
Chemical demulsifiers: surface-acting
compounds that neutralize emulsifying agent stabilizing effect.
Emulsion separation time:
hours to days = “stable” or “tight”; minutes = “loose”.
Aromatic content in crude
reduces emulsification.
Stability measured with a
bottle test (estimates demulsifier phase separation time).
Mechanical emulsion-breaking: free water knockout
drums/separators/desalters/settling tanks.
Emulsion prevention:
reduce solids/chemicals/acids (make very tight emulsions)/mixing/turbulence.
Macroemulsion
& microemulsion differences because of formation and stability
differences.
Macroemulsion: drop size >0.1 micrometer and
will separate (thermodynamically unstable).
Most oilfield macro droplet
coalescence can be reduced through a stabilization mechanism.
Microemulsion: drop size <10 nanometers, separate
(thermodynamically stable).
Emulsion Separation
Index Test (ESI): quantitative
method for lab demulsifier testing (I-569).
…measure water amount separated
at 5, 10, 15, 20 min; then 20 min centrifuged.
…bottle tests have a “qualitative”
edge (due to sampling/operator/measurement error).
…uses dead crude (yet fresh
emulsion samples to minimalize error).
Calculating ESI = [(Sum
of Volume Separated with time)]/[(%BS&W)(# tests)]
Example: ESI = [0 +
4 + 12 + 19 + 25]/[(25)(5)] = 48% water
separation
Monday, April 9, 2018
PEH Volume I Chapter 11: Phase Behavior
I've recently added a page to the Guidebook on Hydrates. Prior editions had the basics, but I found over time I wanted more detail on this complicated subject.
C1-3: Math
C4: Fluid Sampling
C5: Gas Properties
C6: Oil Correlations
C7: Thermo/Phase
C8: Phase Diagrams
C9: Asphaltene/Wax
C10: Produced Water
C11: Phase Behavior
C12: Emulsions
C13: Rock Properties
C14: Permeability
C15: Relative Permeability
C16: Economics
C17-18: Law
Hydrates: the most common solid-phase flow-assurance problem.
H2O & HC typically have 2 separate phases…because H2O bonds >> strength than HC bonds.
C1-3: Math
C4: Fluid Sampling
C5: Gas Properties
C6: Oil Correlations
C7: Thermo/Phase
C8: Phase Diagrams
C9: Asphaltene/Wax
C10: Produced Water
C11: Phase Behavior
C12: Emulsions
C13: Rock Properties
C14: Permeability
C15: Relative Permeability
C16: Economics
C17-18: Law
Hydrates: the most common solid-phase flow-assurance problem.
H2O & HC typically have 2 separate phases…because H2O bonds >> strength than HC bonds.
Hydrates are found
at Low Temperature and High Pressure.
…OR in small-sized HC < n-pentane
size (I-501).
3 hydrate
structures common in HC yet some are unknown (I-508).
Intense variables:
T, P, and compositions.
Gibbs phase
rule (I-335).
F = C – P + 2 used
for:
…how many
intensive variables important in phase equilibria.
…for small
number of components.
…insight to max
number phases that can form.
…insight to
number of intensive properties independently specified.
Example: 1 phase, 1 component: only 2 intensive
properties can be specified (degree of freedom 2).
Example: 3 phases, 2 components: only 1 intensive
property can be specified.
Gibbs P, T diagrams (I-512; semilog plots for nearly
straight lines).
2-component system: “area”. 3-component
system: “line”. 4-component system: “point”.
Single NG
components Hydrate for 3-phase conditions (CH4, etc. Table 11.6).
Water Content
(lbm) per HC wet gas (MMscf) 60 °F,
14.7psia; correct for salinity, gravity (I-502 Fig. 11.1).
4 Types of
H2O-HC Equilibrium PT Diagrams that include hydrates (I-509-512).
1. gases or vapors (say CH4, N2).
2. gas + single condensate + water (HC may be vapor or
liquid).
3. gas + mixed oil/condensate + water.
4. H2O-HC hydrate + inhibitors (MeOH, MEG, salts; note
methanol most economical).
Hand Calculatable:
3-phase Lw-H-V system hydrate formation or wet-gas expansion through
valves.
NOT hand calculable: Lw-H-Lh, I-H-V, 4-phase BUT a Lw-H-V
hand calcs can check computer quality.
Hammerschmidt Expression
for inhibitors finds ΔT (65-X °F)
= 2,335W / (100M – MW) (I-516, 521).
ΔT = hydrate temperature depression and constant
regardless of pressure (65 °F –
T °F).
W = weight % of inhibitor (free-water phase) shifting Lw-H-V
line left below lowest operating temperature.
M = molecular weight of inhibitor (M = 32 for MeOH, 62.07
for MEG).
Hammerschmidt
calculation examples:
ΔT = 2,335W / 100M – MW = 2,335(25) / 100(32) – 32(25) =
24 °F.
W = 100MΔT / MΔT +2,335 = 100(32)24 / (32)24 +2,335 = 25
%wt (of water + MeOH lbm mix).
1. Find gas gravity, temperature, pressure (of hydrate formation conditions).
2. Find W from the Hammerschmidt expression.
3. Find mass of liquid water, from condensed and liquid
water (lbm water/MMscf of gas).
4. Find rate of MeOH in the aqueous phase W =
MeOH/(H2O+MeOH).
Hydrate
Formation on Expansion Across Valve or Restriction (I-524-528).
Monday, April 2, 2018
PEH Volume I Chapter 10: Produced Water
C1-3: Math
C4: Fluid Sampling
C5: Gas Properties
C6: Oil Correlations
C7: Thermo/Phase
C8: Phase Diagrams
C9: Asphaltene/Wax
C10: Produced Water
C11: Phase Behavior
C12: Emulsions
C13: Rock Properties
C14: Permeability
C15: Relative Permeability
C16: Economics
C17-18: Law
Produced Water Properties (I-466-494):
Meteoric Water = water recently in contact with atmosphere (from surface).
Connate = Original sedimentary interstitial = Fossil water (away from atmosphere since settling).
Juvenile Water = never contacts atmosphere (from deep; mineral diagenesis --> water expulsion.
Water: chemical signature may ID depth (strata).
Water produced: increases as oil produced increases (usually; even primary production).
Water: excellent solvent: reacts to dissolve many phases it contacts.
Scale deposits on ESPs: precipitates due to motor heat.
Reserves typically limited by water handling costs (even secondary & tertiary).
Volatile organic acids: formic, acetic, propionic, butyric.
Dissolved aromatic compounds: benzene, toluene, xylenes (often included in oil carryover by law).
Hydrocarbon carryover in produced water: important issue for surface engineers.
Common scales: calcium carbonate, calcium sulfate, barium sulfate, iron sulfide, iron carbonate.
Scale inhibition: uses organic compounds to slow growth sites.
Scale inhibition: lab experiments, not just computers, needed to select inhibition compounds.
Corrosion prediction less certain than scale-precipitation predictions.
DST water sample: TDS increase downhole; ideal sample when TDS constant or final water to tool.
Water samples: taken from flowline (above) or wellhead.
Water tests: for compressibility, density, FVF, resistivity, surface tension, viscosity, pH, pE.
It's a good idea to review this section in the Handbook and highlight if unfamiliar.
C4: Fluid Sampling
C5: Gas Properties
C6: Oil Correlations
C7: Thermo/Phase
C8: Phase Diagrams
C9: Asphaltene/Wax
C10: Produced Water
C11: Phase Behavior
C12: Emulsions
C13: Rock Properties
C14: Permeability
C15: Relative Permeability
C16: Economics
C17-18: Law
Produced Water Properties (I-466-494):
Meteoric Water = water recently in contact with atmosphere (from surface).
Connate = Original sedimentary interstitial = Fossil water (away from atmosphere since settling).
Juvenile Water = never contacts atmosphere (from deep; mineral diagenesis --> water expulsion.
Water: chemical signature may ID depth (strata).
Water produced: increases as oil produced increases (usually; even primary production).
Water: excellent solvent: reacts to dissolve many phases it contacts.
Scale deposits on ESPs: precipitates due to motor heat.
Reserves typically limited by water handling costs (even secondary & tertiary).
Volatile organic acids: formic, acetic, propionic, butyric.
Dissolved aromatic compounds: benzene, toluene, xylenes (often included in oil carryover by law).
Hydrocarbon carryover in produced water: important issue for surface engineers.
Common scales: calcium carbonate, calcium sulfate, barium sulfate, iron sulfide, iron carbonate.
Scale inhibition: uses organic compounds to slow growth sites.
Scale inhibition: lab experiments, not just computers, needed to select inhibition compounds.
Corrosion prediction less certain than scale-precipitation predictions.
DST water sample: TDS increase downhole; ideal sample when TDS constant or final water to tool.
Water samples: taken from flowline (above) or wellhead.
Water tests: for compressibility, density, FVF, resistivity, surface tension, viscosity, pH, pE.
It's a good idea to review this section in the Handbook and highlight if unfamiliar.
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