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(1)

Flow Assurance

서유택

(2)

Gathering system

Small ID induces lots of energy loss

→ larger pressure drop

(3)

Pressure drop vs. Flowrate in oil field flowlines

△Ptotal = △Pfriction + △Pelevation + △Prestriction

(4)

Darcy – Weisbach Formula

• Pressure drop expressed in feet of fluid head ℎ

𝑓𝑡

= 𝑓 𝐿 𝑣

2

𝐷 2𝑔

• Pressure drop expressed in psi

△ 𝑃 = ρ 𝑓 𝐿 𝑣

2

144 𝐷 2𝑔

g: correction factor

not gravity acceleration ( = 32.2 ft/s2 = 9.81 m/s2)

(5)

Flow regime in pipe

• Gas dominant stream is mostly turbulent

• Flow regime determined by Reynolds number

(6)

Reynolds number

• Dimensionless parameter

: Ratio of Inertia forces to Viscous forces

• Re < 2000 = Laminar flow

𝐿𝑖𝑞𝑢𝑖𝑑: 𝑅𝑒 = 92.1 𝑆𝐺

𝐿

𝑄

𝐵𝑃𝐷

𝑑 𝜇

𝐺𝑎𝑠: 𝑅𝑒 = 20100 𝑆𝐺

𝐺

𝑄

𝑀𝑀𝐶𝐹𝐷

𝑑 𝜇

d: inches, μ: centipoise

(7)

Friction factor

• f = Dimensionless factor of proportionality

fm = Moddy friction factor

ff = Fanning fraction factor (ff =1/4 fm)

• Laminar flow: f

m

= 64 / Re

• For transitional and turbulent flow

- fm a function of Re

- Relative roughness: ε / D

• For complete turbulence

- fm a function of ε / D only

(8)
(9)
(10)
(11)

Pressure drop: Laminar flow (Re < 2000)

• Liquid

∆𝑃

𝑝𝑠𝑖

= 0.00068 𝜇

𝑐𝑝

𝐿

𝑓𝑡

𝑉

𝑓𝑡/𝑠𝑒𝑐

𝑑

𝑖𝑛2

∆𝑃

𝑝𝑠𝑖

= 7.95 × 10

−6

𝜇

𝑐𝑝

𝐿

𝑓𝑡

𝑄

𝐵𝑃𝐷

𝑑

𝑖𝑛4

• Gas

∆𝑃

𝑝𝑠𝑖

= 0.040 𝜇

𝑐𝑝

𝐿

𝑓𝑡

𝑇

𝑜𝑅

𝑍𝑄

𝑀𝑀𝐶𝐹𝐷

𝑃

𝑝𝑠𝑖

𝑑

𝑖𝑛4
(12)

Pressure drop: Transitional and Turbulent

• Liquid

∆𝑃

𝑝𝑠𝑖

= 11.5 × 10

−6

𝑓

𝑚

𝐿

𝑓𝑡

𝑄

𝐵𝑃𝐷2

𝑆𝐺

𝐿

𝑑

𝑖𝑛5

• Gas

𝑃

12

−𝑃

22

= 25.1 𝑓

𝑚

𝐿

𝑓𝑡

𝑄

𝑀𝑀𝐶𝐹𝐷2

𝑆𝐺

𝐺

𝑍𝑇

𝑅

𝑑

𝑖𝑛5
(13)

Exercise Δ P: Liquid flow in Pipe

• What is the friction pressure drop in 10,000 ft of 2 inch ID pipe flowing 50 BPD of 35

o

API crude oil (μ=1.2 cp and SG

L

=0.85) ?

1. First calculate Reynold’s number to determine flow regime

: Re = 1,631 so flow is Laminar

2. Use the equation for Laminar

∆𝑃𝑝𝑠𝑖= 7.95 × 10−6𝜇𝑐𝑝𝐿𝑓𝑡𝑄𝐵𝑃𝐷 𝑑𝑖𝑛4

∆𝑃𝑝𝑠𝑖= 0.3 psi

(14)

Exercise: Increasing flow rate 3000 BPD

1. First calculate Reynold’s number to determine flow regime

: Re = 97,856, Re > 2000 so flow is Non-Laminar

2. Use the equation for Turbulent-Transitional

∆𝑃𝑝𝑠𝑖= 11.5 × 10−6 𝑓𝑚𝐿𝑓𝑡𝑄𝐵𝑃𝐷2 𝑆𝐺𝐿 𝑑𝑖𝑛5

3. Determine fm using chart fm= 0.022

∆𝑃𝑝𝑠𝑖= 605 psi

(15)
(16)

Pipeline sizing Summary

(17)

Pipeline installation

(18)

What if pipeline is not horizontal?

(19)

Pressure drop due to Elevation

• Liquid: ΔP due to Elevation

∆𝑃𝐸(𝑝𝑠𝑖) = 𝜌𝐿(𝑙𝑏/𝑓𝑡

2)𝐻𝐸(𝑓𝑡)

144 = 62.4𝑆𝐺𝐿𝐻𝐸(𝑓𝑡)

144

∆𝑃𝐸(𝑝𝑠𝑖) = 0.433 𝑆𝐺𝐿𝐻𝐸(𝑓𝑡)

• Gas: ΔP due to Elevation

∆𝑃

𝐸(𝑝𝑠𝑖)

= 𝜌

𝐺(𝑙𝑏/𝑓𝑡2)𝐻𝐸(𝑓𝑡)

144 = 2.70 𝑆𝐺

𝐺

𝑃

𝑝𝑠𝑖

/𝑇

𝑜𝑅

𝑍𝐻

𝐸(𝑓𝑡)

144

∆𝑃

𝐸(𝑝𝑠𝑖)

= 0.188 𝑆𝐺

𝐺

𝑃

𝑝𝑠𝑖

𝑇

𝑜𝑅

𝑍 𝐻

𝐸(𝑓𝑡)
(20)

Not always true for gas flow

• Big liquid droplets for annular flow

(21)

Pressure drop for Wet gas

• Sum the “Ups”

(22)

Estimating ΔP without using Friction Factor

• Empirical equations

- Useful for quick calculation before use of PCs - Commonly accepted empirical equations

: Hazen-Williams empirical equation (Liquid flow)

∆𝑃 = 0.7 × 10−6𝑄1.85𝐿 𝑆𝐺𝐿 𝑑4.87

(∆𝑃 𝑖𝑛 𝑝𝑠𝑖, 𝑄 𝑖𝑛 𝐵𝐿𝑃𝐷, 𝐿 𝑖𝑛 𝑓𝑒𝑒𝑡, 𝑑 = 𝐼𝐷 𝑖𝑛 𝑖𝑛𝑐ℎ𝑒𝑠) : Weymouth formula (gas flow)

𝑃22 = 𝑃12 − 0.8 𝐿𝑓𝑡𝑇𝑅𝑍 𝑆𝐺𝐺𝑄𝑀𝑀𝐶𝐹𝐷2 𝑑𝑖𝑛5.334

- most common for oil field use

- good for IDs between 0.75 inch & 16 inch - at Laminar rates, calculated ΔP is too low : Panhandle empirical equation (gas flow)

(23)

Panhandle: A & B Empirical equation

• For estimating ΔP without friction factor A: 𝑄

𝑀𝑀𝐶𝐹𝐷

=

0.020 𝐸 𝑃12−𝑃22 0.51𝑑2.62

𝑆𝐺𝐺0.853𝑧𝑇𝑜𝑅𝐿𝑚𝑖 0.539

- For IDs between 6 inch and 24 inch - Re between 5*106 and 15*106

B: 𝑄

𝑀𝑀𝐶𝐹𝐷

=

0.028 𝐸 𝑃12−𝑃22 0.51𝑑2.53

𝑆𝐺𝐺0.961𝑧𝑇𝑜𝑅𝐿𝑚𝑖 0.51

- For IDs between 6 inch and 24 inch - Re > 15*106

ΔP in psi, Q in MMCFD, Lmi in miles, d = ID in inches E factor : E = 1.00 for new pipe

= 0.95 for good condition

= 0.92 for average condition

= 0.85 for old pipe

= 0.75 for corroded pipe

(24)
(25)

Pressure drop in pipe: Two phase flow

• With liquid and gas both flowing

- Two phase flow - Three phase flow

• Horizontal flow patterns

- Noise produced with bubbles

- Using superficial velocities for gas and liquid

(26)

Two-phase horizontal flow regime

(27)

Vertical two-phase flow regimes

(28)

Two-phase vertical flow regimes

(29)

Pressure drop for two-phase flow

• Very complex: errors ≈ 20% common

- Use simulation software and experience

• API RP 14 E gives following simplified method

- Assumes: ΔP < 10%, bubble / mist flow, f=0.015 Δ𝑃 = 5 × 10−8 𝐿 𝑊2

𝑑5 𝜌𝑚𝑖𝑥

where, W= 3180 𝑄𝑀𝑀𝐶𝐹𝐷𝑆𝐺𝐺 + 14.6 𝑄𝐵𝑃𝐷𝑆𝐺𝐿 𝑎𝑛𝑑 𝜌𝑚𝑖𝑥 = 12409 𝑆𝐺𝐿𝑃 + 2.7 𝑅𝑠𝑐𝑓/𝑏𝑏𝑙𝑆𝐺𝐺𝑃

198.7 𝑃 + 𝑅𝑠𝑐𝑓/𝑏𝑏𝑙 𝑇 𝑧

(30)

Two phase flow: High GOR > 10,000 ft

3

/bbl

• Use gas equations but change SG

G

to :

𝑆𝐺

𝑚𝑖𝑥

=

𝑆𝐺

𝐺

+ 4591 𝑆𝐺

𝐿

𝑅

𝑠𝑐𝑓/𝑏𝑏𝑙

1 + 1123

𝑅

𝑠𝑐𝑓/𝑏𝑏𝑙

If GOR < 10,000 scf/bbl, use two-phase correlations

(31)

AGA: Recommended multiphase Δ P calculations

(32)

Pressure drop through valves and fittings

(33)

Pressure drop through valves and fittings

(34)

Pressure drop through valves and fittings

• Resistance coefficients: K

r

• Flow coefficients: liquid – C

v

, Gas – C

g

• Equivalent length: L

E
(35)

Darcy’s Law for valves and fittings

• Resistance coefficient: K

r

∆𝐻 = 𝐾

𝑟

𝑣

2

2 𝑔 , 𝑤ℎ𝑒𝑟𝑒 𝐾

𝑟

= 𝑓 𝐿 𝐷

• Liquid

∆𝑃

𝑝𝑠𝑖

= 0.958 × 10

−6

𝐾

𝑟

𝑄

𝐵𝑃𝐷2

𝑆𝐺

𝐿

𝑑

4

• Gas

𝑃

12

− 𝑃

22

= 2.09 𝐾

𝑟

𝑄

𝑀𝑀𝐶𝐹𝐷2

𝑆𝐺

𝐺

𝑧 𝑇

𝑜𝑅

𝑑

4
(36)

Resistance coefficients

(37)

Darcy’s law for valves and fittings

• Flow coefficient: C

v

and C

g

: a relative measure of its efficiency at allowing fluid flow

• Liquid

∆𝑃

𝑝𝑠𝑖

= 8.5 × 10

−4

𝑄

𝐵𝑃𝐷2

𝑆𝐺

𝐿

𝐶

𝑣2

• Gas

𝑃

12

− 𝑃

22

= 1.869 𝑄

𝑀𝑀𝐶𝐹𝐷2

𝑆𝐺

𝐺

𝑧 𝑇

𝑜𝑅

𝐶

𝑔2
(38)

Relationship between K

r

and C

v

𝐶

𝑣

= 29.9 𝑑

2

𝐾

𝑟

𝐾

𝑟

= 894 𝑑

4

𝐶

𝑣2
(39)

Equivalent lengths

• The pressure drop in a system component such as valve and fittings can be converted to the "equivalent length" of a pipe or tube that would give the same pressure loss.

𝐿

𝐸

= 𝐾

𝑟

𝑑 12 𝑓

𝑚

𝐿

𝐸

= 74.5 𝑑

5

𝑓

𝑚

𝐶

𝑣2
(40)
(41)

Gate valve

(42)

Globe valve

(43)

Thank you

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