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Equations: The rig and the drilling process

The equations of the “The rig and the drilling process” lessons in “Drilling engineering”, with their conditions and units, and what each symbol means in them.

Annular volume and lag time
Va=π4∑i(Di2−di2)Li,tlag=VaQV_a = \frac{\pi}{4}\sum_i \left(D_i^2 - d_i^2\right) L_i, \qquad t_{lag} = \frac{V_a}{Q}

SI. It is handy to calculate the annular capacity in litres per metre as π4(D2−d2)⋅10−3\frac{\pi}{4}(D^2 - d^2)\cdot 10^{-3} with the diameters in millimetres

Holds when: The lengths of the intervals are measured along the hole, not vertically, because the mud travels the whole path. The mud and the cuttings move at the same average speed. In reality the cuttings lag behind the mud, especially in deviated holes. The open hole has its nominal (design) diameter. Washouts (places where the hole is wider than the bit) add volume and time, so we check the calculation with a tracer. The pump rate is constant and known. We calculate it from the number of pump strokes and the volume of one stroke, allowing for the volumetric efficiency (the share of the stroke volume that the pump really delivers).

How a well is drilled: the process and the people involved →
Mechanical, technical and commercial drilling speed
vmech=Htbot,vtech=720 HTprod,vcom=720 HTcalv_\text{mech} = \frac{H}{t_\text{bot}}, \qquad v_\text{tech} = \frac{720\,H}{T_\text{prod}}, \qquad v_\text{com} = \frac{720\,H}{T_\text{cal}}

metres and hours; speeds in m/h and metres per rig-month (m/rig-month)

Holds when: TprodT_\text{prod} and TcalT_\text{cal} do not include preparatory work, rig-up or testing. A speed that includes them is called the cycle speed. For a group of wells, use the total footage and the total time. The trip-averaged rate of penetration describes one bit. It is the footage of a bit run divided by the drilling and tripping time of that run (measures of bit performance).

Drilling time and cost →
Cost of a well by type of cost
C=Clump+r T+∑jcj LjC = C_\text{lump} + r\,T + \sum_j c_j\,L_j

any currency; in the example, thousand US dollars and days

Holds when: TT is the number of days from the time estimate. The drilling contract decides how the time of repairing the rig is paid. The boundary between the types is not sharp: bits depend on both metres and time, and mud consumption depends on the volume of the hole and on losses. Prices are those of the date of the estimate. For a programme lasting several years, we allow for rising prices (escalation).

Drilling time and cost →
Cost of an event and the mean contingency from a risk register
ΔCk=r Δtk+ck,E[ΔC]=∑kpk ΔCk\Delta C_k = r\,\Delta t_k + c_k, \qquad \mathrm{E}[\Delta C] = \sum_k p_k\,\Delta C_k

thousand US dollars and days

Holds when: The events are independent: each happens at most once, and its consequences do not depend on the others. Linked events are combined, or they are given by a conditional probability. An example is lost circulation, after which stuck pipe is more likely. The register is incomplete, so we add a contingency for what it does not cover. Means add up whatever the relation between the events, but P90 values do not. We find the P90 of a sum from the whole distribution, by listing the combinations or by simulation (why P90 values are not added).

Drilling time and cost →
The learning curve (Brett–Millheim model)
tn=C1 eC2(1−n)+C3t_n = C_1\,\e^{C_2(1-n)} + C_3

days

Holds when: The wells are of one type in one area, with one rig and one contractor. A break in the work, a change of crew or a change of casing programme sets the series back. We fit the constants to the actual wells of the series. It is more reliable to estimate C3C_3 separately, from the technical limit or the best composite well (fitting the curve). Non-productive time improves less with learning than productive time, so it is often analysed separately.

Drilling time and cost →
Complete or abandon
Vwell>Ccompl−CabandV_\text{well} > C_\text{compl} - C_\text{aband}

thousand US dollars at the date of the decision

Holds when: The cost of drilling to the planned depth has already been spent and does not depend on the decision, so it is not part of the comparison (sunk cost). The abandonment of a completed well at the end of its life is included in VwellV_\text{well}. It comes years later, so it weighs less after discounting (converting future money into today's value). If the well is also needed for other purposes, such as injection or observation, add their value to VwellV_\text{well}.

Drilling time and cost →
Required electric power and fuel consumption
Nel=1ηdrive(pQηmech+Mω)+Naux,Gf=gf Nel t\begin{gathered} N_{\text{el}} = \frac{1}{\eta_{\text{drive}}}\left(\frac{pQ}{\eta_{\text{mech}}} + M\omega\right) + N_{\text{aux}},\\ G_{\text{f}} = g_{\text{f}}\,N_{\text{el}}\,t \end{gathered}

kW, MPa × L/s = kW, kN·m × rad/s = kW

Holds when: The loads are constant during the calculation time. In reality they change with connections, circulating and trips, so the daily consumption is calculated from a load schedule. The specific fuel consumption (the fuel burned per kilowatt-hour) depends on the generator load. For modern diesel generators near the rated load it is about 0.2 kg/(kW·h), and noticeably more at a light load.

Drilling rig: power and hoisting systems →
Block efficiency of the reeving
η=Wn Ffl=Kn−1Kn n (K−1)\eta = \frac{W}{n\,F_{\text{fl}}} = \frac{K^n - 1}{K^n\,n\,(K - 1)}

dimensionless

Holds when: This is the ordinary rig reeving: the dead line passes over the stationary sheave of the crown block, and the rope goes round as many rotating sheaves as there are lines strung. If there are extra rotating sheaves in the path of the rope, their total number SS replaces nn in the exponent of the denominator, giving KSK^S. The block moves upward at constant speed. Acceleration, braking and jerks add dynamic loads that the formula does not include. KK is a calculated value. It covers friction in the bearings and the loss in bending the rope. The sheave manufacturer may give its own value.

Drilling rig: power and hoisting systems →
Tension in the fast line and the dead line
Ffl=Wη n,Fdl=WnF_{\text{fl}} = \frac{W}{\eta\,n}, \qquad F_{\text{dl}} = \frac{W}{n}

any units of force

Holds when: The dead line does not move, so its tension is taken as static, W/nW/n. When the block moves, friction in the sheaves makes the tension smaller when hoisting and larger when lowering (see the advanced section). For the derrick load when hoisting, W/nW/n errs on the safe side. The ratio Ffl/W=1/(ηn)F_{\text{fl}}/W = 1/(\eta n) is called the fast line factor.

Drilling rig: power and hoisting systems →
Design factor of the drilling line
kdf=RFflk_{\text{df}} = \frac{R}{F_{\text{fl}}}

any identical units of force

Holds when: The minimum values by API RP 9B are: 3 for the drilling line while drilling and tripping; 2 when running casing, when working stuck pipe and in other rare operations; and 2.5 for the line used to raise the mast. For a worn rope and under shock loads, the actual factor is lower than the calculated one. Work near the minimum is possible only with a sound line and equipment, and without jerks.

Drilling rig: power and hoisting systems →
Power at the drawworks drum and hoisting speed
Ndrum=Ffl vfl=Wvη,vfl=n v,Nin=Ndrumηdw\begin{gathered} N_{\text{drum}} = F_{\text{fl}}\,v_{\text{fl}} = \frac{W v}{\eta}, \qquad v_{\text{fl}} = n\,v,\\ N_{\text{in}} = \frac{N_{\text{drum}}}{\eta_{\text{dw}}} \end{gathered}

kN × m/s = kW

Holds when: The motion is steady. Accelerating a string of hundreds of tonnes needs extra power, so acceleration and braking are made smooth. When lowering, energy flows the other way: the load itself pulls the line, and the brakes or the motors in braking mode absorb the power WvWv (less friction).

Drilling rig: power and hoisting systems →
Derrick load
Fder=W+Ffl+Fdl=W 1+η+η nη nF_{\text{der}} = W + F_{\text{fl}} + F_{\text{dl}} = W\,\frac{1 + \eta + \eta\,n}{\eta\,n}

any identical units of force

Holds when: The fast line and the dead line run down from the crown block almost vertically. Slanting lines and wind add horizontal forces, which are allowed for in the design of the derrick itself. The dead line is taken as static (W/nW/n). The load is shared unevenly among the legs of the derrick (see the advanced section).

Drilling rig: power and hoisting systems →
Work of the drilling line in a full round trip
Trt=D (Lst+D) w+4D (Wtrav+C/2)9807T_{\text{rt}} = \frac{D\,(L_{\text{st}} + D)\,w + 4D\,(W_{\text{trav}} + C/2)}{9807}

kN·m divided by 9807 kN·m per t·km (tonne-force × kilometre)

Holds when: The drill pipe is taken to reach the bottom, and the excess weight CC accounts for the heavy bottom part. For each stand, the travelling equipment moves up and down over the length of the stand when hoisting, and the same when lowering. This gives 4D4D in total per round trip. Friction is the same when lowering and when hoisting. Accelerations, vibrations and drag in a deviated hole are not included. This is a comparative measure of wear, not exact work.

Drilling rig: power and hoisting systems →
Line work in drilling, running casing and a short trip
Tdrill=3[Trt(D2)−Trt(D1)],Tshort=Trt(Dlow)−Trt(Dup),Tcsg=D (Ljt+D) wcsg+4D Wtrav2⋅9807\begin{gathered} T_{\text{drill}} = 3\left[T_{\text{rt}}(D_2) - T_{\text{rt}}(D_1)\right],\\ T_{\text{short}} = T_{\text{rt}}(D_{\text{low}}) - T_{\text{rt}}(D_{\text{up}}),\\ T_{\text{csg}} = \frac{D\,(L_{\text{jt}} + D)\,w_{\text{csg}} + 4D\,W_{\text{trav}}}{2\cdot 9807} \end{gathered}

t·km; depths and lengths in m, weights in kN and kN/m

Holds when: Drilling goes in a cycle: drill the length of a joint or stand, pick up off bottom, ream (work the bit through the new section again), pick up for the connection, make the connection, and lower. In this cycle the line does work equal to three full round trips over the increase in depth. If the string is not reamed or lifted before the connection, it is two. In a short trip, the whole string is raised and lowered over the interval between two depths. The work is exactly the difference between the work of full round trips at those depths. Casing is only run in, so the work is half that of a full round trip. There are no collars in a casing string.

Drilling rig: power and hoisting systems →
Equivalent derrick load and its utilisation factor
Feq=4(W4+Wn)=W n+4n,Eder=FderFeq=1+η+η nη (n+4)\begin{gathered} F_{\text{eq}} = 4\left(\frac{W}{4} + \frac{W}{n}\right) = W\,\frac{n + 4}{n},\\ E_{\text{der}} = \frac{F_{\text{der}}}{F_{\text{eq}}} = \frac{1 + \eta + \eta\,n}{\eta\,(n + 4)} \end{gathered}

any identical units of force

Holds when: The derrick has four legs, and the load from the working lines is shared equally among them. The dead line is anchored at one leg and the drawworks is midway between two others. For another arrangement the distribution is different, and masts have their own scheme.

Drilling rig: power and hoisting systems →
Output of a mud pump per stroke and per unit of time
Vstk=3⋅π4 d2L ηv  (triplex),Vstk=π2(2d2−drod2)L ηv  (duplex),Q=Vstk n60\begin{gathered} V_{\text{stk}} = 3\cdot\frac{\pi}{4}\,d^2 L\,\eta_v \ \ \text{(triplex)}, \qquad V_{\text{stk}} = \frac{\pi}{2}\left(2d^2 - d_{\text{rod}}^2\right) L\,\eta_v \ \ \text{(duplex)},\\ Q = \frac{V_{\text{stk}}\,n}{60} \end{gathered}

SI. It is convenient to take dd and LL in decimetres, because then VstkV_{\text{stk}} comes out directly in litres

Holds when: The volume swept by the piston is calculated from the full stroke. In a duplex pump the return stroke displaces the volume of the ring-shaped space between the liner and the rod. The volumetric efficiency accounts for leakage through the valves and pistons, incomplete filling of the cylinders and compression of gas in the mud. For a pump in good order with a charge pump it is close to 1. For a worn pump it falls to 0.9 and below. With several pumps the outputs add up, and the total counter counts the strokes of all the pumps.

Rig circulating and rotary systems →
Allowable liner pressure and the power limit
pmax⁡=Frodπd2/4,Nhyd=p Q≤ηmech Ndrivep_{\max} = \frac{F_{\text{rod}}}{\pi d^2/4}, \qquad N_{\text{hyd}} = p\,Q \le \eta_{\text{mech}}\,N_{\text{drive}}

MN/m² = MPa; MPa × L/s = kW

Holds when: The strength of the fluid end, and not only the rod load, may also limit the pressure. For small liners the rated pressure can be lower than the one calculated from the rod load. Pump data sheets give the allowable pressure and the output at the highest stroke rate for each liner in a table. The formula explains where these numbers come from.

Rig circulating and rotary systems →
Strokes to the bit and up the annulus
Zbit=VstringVstk,Zann=VannVstk,t=VQZ_{\text{bit}} = \frac{V_{\text{string}}}{V_{\text{stk}}}, \qquad Z_{\text{ann}} = \frac{V_{\text{ann}}}{V_{\text{stk}}}, \qquad t = \frac{V}{Q}

SI; the volume of the hole and of the pipe is π4(D2−d2)\frac{\pi}{4}(D^2 - d^2) per metre of length

Holds when: The pipe and the hole have their nominal diameters. Washouts increase the volume of the annulus, so the actual time is checked with a tracer. The mud is incompressible and is not lost anywhere. With lost circulation or an influx the volumes stop adding up, and that is the warning sign.

Rig circulating and rotary systems →
Power of rotating the string
Nrot=M ω,ω=2π nrot60N_{\text{rot}} = M\,\omega, \qquad \omega = \frac{2\pi\,n_{\text{rot}}}{60}

kN·m × rad/s = kW

Holds when: The rotation is steady. The torque at the surface is the sum of the torque at the bit and the friction of the string against the walls. In a deviated well the friction is usually the larger part (drag and torque). The power at the input of the drive is higher by its efficiency.

Rig circulating and rotary systems →

Symbols

SymbolMeaning and context
720720
CC
C1C_1
  • by how much the first well exceeds the limit: t1=C1+C3t_1 = C_1 + C_3, dDrilling time and cost
C2C_2
C3C_3
CabandC_\text{aband}
CcomplC_\text{compl}
cjc_j
  • unit price of the jj-th material: a metre of casing, a bit, a tonne of cement, US$ thousand per unitDrilling time and cost
ckc_k
  • direct cost of the event: materials, fishing (recovering stuck or lost tools), tools left in the hole, US$ thousandDrilling time and cost
ClumpC_\text{lump}
  • lump-sum costs: the site, mobilisation, wellhead equipment, service operations paid per job, US$ thousandDrilling time and cost
dd
DD
did_i
DiD_i
  • diameter of the hole in the ii-th interval. In open hole (the part with no casing), use the bit diameter, or the real diameter from the caliper log (a log that measures the hole diameter). In cased hole, use the inside diameter of the casing, mHow a well is drilled: the process and the people involved
d, drodd,\ d_{\text{rod}}
EderE_{\text{der}}
E[ΔC]\mathrm{E}[\Delta C]
FderF_{\text{der}}
FdlF_{\text{dl}}
FeqF_{\text{eq}}
FflF_{\text{fl}}
FrodF_{\text{rod}}
Gf, gf, tG_{\text{f}},\ g_{\text{f}},\ t
HH
ΔCk\Delta C_k
Δtk\Delta t_k
KK
kdfk_{\text{df}}
LL
LiL_i
LjL_j
Ljt, wcsgL_{\text{jt}},\ w_{\text{csg}}
LstL_{\text{st}}
MM
M, ωM,\ \omega
  • torque and angular speed of the top drive or rotary table (ω=2πnrot/60\omega = 2\pi n_{\text{rot}}/60 at a rotary speed nrotn_{\text{rot}} rpm), kN·m, rad/sDrilling rig: power and hoisting systems
nn
NauxN_{\text{aux}}
NdrumN_{\text{drum}}
NelN_{\text{el}}
NhydN_{\text{hyd}}
Nin, ηdwN_{\text{in}},\ \eta_{\text{dw}}
NrotN_{\text{rot}}
pkp_k
pmax⁡p_{\max}
p, Qp,\ Q
QQ
rr
RR
TT
tbott_\text{bot}
TcalT_\text{cal}
TcsgT_{\text{csg}}
TdrillT_{\text{drill}}
tlagt_{lag}
tnt_n
TprodT_\text{prod}
TrtT_{\text{rt}}
TshortT_{\text{short}}
t, V, Qt,\ V,\ Q
VaV_a
VannV_{\text{ann}}
vmechv_\text{mech}
VstkV_{\text{stk}}
VstringV_{\text{string}}
vtech, vcomv_\text{tech},\ v_\text{com}
VwellV_\text{well}
  • the value of the well's production: the NPV (net present value, the value today) of its future cash flows, leaving out the costs already spent and the cost of completion, US$ thousandDrilling time and cost
v, vflv,\ v_{\text{fl}}
ww
WW
WtravW_{\text{trav}}
W, n, ηW,\ n,\ \eta
W, n, η, FderW,\ n,\ \eta,\ F_{\text{der}}
W, Ffl, FdlW,\ F_{\text{fl}},\ F_{\text{dl}}
W, Ffl, η, nW,\ F_{\text{fl}},\ \eta,\ n
Zbit, ZannZ_{\text{bit}},\ Z_{\text{ann}}
η\eta
η, n\eta,\ n
ηdrive\eta_{\text{drive}}
ηmech\eta_{\text{mech}}
ηmech, Ndrive\eta_{\text{mech}},\ N_{\text{drive}}
ηv\eta_v
ω, nrot\omega,\ n_{\text{rot}}