pressure loss in unsteady annular channel flow

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Pasquini, Enrico 3/19/2018 Pasquini, Enrico Pressure Loss in Unsteady Annular Channel Flow 1

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Page 1: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Pasquini, Enrico

Pressure Loss in Unsteady Annular Channel Flow

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Page 2: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

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2

3

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Introduction to the problem of unsteady pressure loss

Pressure loss in unsteady annular channel flow

Summary & Outlook

Plane channel approximation

2

Outline

Page 3: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

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2

3

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Introduction to the problem of unsteady pressure loss

Pressure loss in unsteady annular channel flow

Summary & Outlook

Plane channel approximation

3

Outline

Page 4: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Introduction to the problem of unsteady pressure loss

β€’ What is an annular channel?

β€’ An annular channel is created by mounting a cylinder within a pipe:

β€’ Key design parameter: radius ratio 𝜚 =π‘Ÿπ‘–

π‘Ÿπ‘œ

β€’ Radius ratio ranging from 0 < 𝜚 ≀ 1, depending on application

β€’ 𝜚 = 0: circular pipe without internal cylinder

β€’ 𝜚 β†’ 1: vanishing gap height β„Ž = π‘Ÿπ‘œ βˆ’ π‘Ÿπ‘–, typically found in sealing gaps

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Page 5: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Introduction to the problem of unsteady pressure loss

β€’ Hydraulic engineering problem: calculation of pressure loss Δ𝑝 for a given area-

averaged flow velocity 𝑒 or flow rate 𝑄 (also vice versa)

β€’ CFD simulations are too time-consuming for design studies β†’ 1D simulation

β€’ For steady laminar flow, an analytical expression for Δ𝑝 𝑒 is known:

Δ𝑝

Δ𝑧=πœ‚

π‘Ÿπ‘œ2

8

1 + 𝜚2 +1 βˆ’ 𝜚2

ln 𝜚

𝑒

β€’ For unsteady laminar flow, no analytical expression is known yet

β€’ First guess: Take the instantaneous value of 𝑒 𝑑 and calculate the unsteady

pressure loss based on the formula above

β€’ This method is referred to as the quasi steady approach

β€’ Quasi steady approach gives exact results for unsteady flows with relatively low

frequencies

β€’ Quasi steady approach fails to predict pressure loss in highly dynamic unsteady

flows

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Page 6: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Introduction to the problem of unsteady pressure loss

β€’ Example for highly dynamic event: Water hammer experiment

β€’ How can unsteady pressure loss be calculated?

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Page 7: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

1

2

3

4

Introduction to the problem of unsteady pressure loss

Pressure loss in unsteady annular channel flow

Summary & Outlook

Plane channel approximation

7

Outline

Page 8: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

β€’ Pressure loss is proportional to wall shear stress

β€’ Wall shear stress is proportional to radial velocity gradient

β€’ First step: Determination of velocity profile based on Navier-

Stokes (NS) equation

β€’ NS equation (axial direction) in cylindrical coordinates:

πœ•π‘’

πœ•π‘‘+1

𝜌

πœ•π‘

πœ•π‘§= 𝜈

πœ•2𝑒

πœ•π‘Ÿ2+1

π‘Ÿ

πœ•π‘’

πœ•π‘Ÿ

β€’ Strategy:

– Perform Laplace transform of NS equation

– Apply boundary conditions (no slip between fluid and

cylinder/pipe walls)

– Solve for π‘’βˆ—

Pressure loss in unsteady annular channel flow

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β„’πœ•π‘’

πœ•π‘‘= π‘ π‘’βˆ—

π‘’βˆ— π‘Ÿπ‘– = π‘’βˆ— π‘Ÿπ‘œ = 0

𝜏 ∝ πœ‚πœ•π‘’

πœ•π‘Ÿ

Δ𝑝

Ξ”π‘§βˆ 𝜏

Page 9: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

β€’ Result: Laplace transform of radial velocity profile π‘’βˆ— as a function of

transformed axial pressure gradient πœ•π‘βˆ—

πœ•π‘§:

π‘’βˆ— π‘Ÿ =1

π‘ πœŒ

πœ•π‘βˆ—

πœ•π‘§

𝐼0 π‘Ÿπ‘ πœˆ

𝐾0 π‘Ÿπ‘œπ‘ πœˆβˆ’ 𝐾0 πœšπ‘Ÿπ‘œ

π‘ πœˆ

βˆ’ 𝐾0 π‘Ÿπ‘ πœˆ

𝐼0 π‘Ÿπ‘œπ‘ πœˆβˆ’ 𝐼0 πœšπ‘Ÿπ‘œ

π‘ πœˆ

𝐼0 πœšπ‘Ÿπ‘œπ‘ πœˆπΎ0 π‘Ÿπ‘œ

π‘ πœˆβˆ’ 𝐼0 π‘Ÿπ‘œ

π‘ πœˆπΎ0 πœšπ‘Ÿπ‘œ

π‘ πœˆ

βˆ’ 1

β€’ For oscillating flow (oscillation frequency 𝑓), the normalized velocity profile

depends on two non-dimensional parameters:

– Gap Womersley number π‘Šπ‘œβ„Ž = β„Žπ‘ 

𝜈= β„Ž

2πœ‹π‘“

𝜈

– Radius ratio 𝜚

β€’ How do changes in gap Womersley number and radius ratio influence the

velocity profile?

Pressure loss in unsteady annular channel flow

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Page 10: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

β€’ Influence of radius ratio 𝜚 on velocity profile (π‘Šπ‘œβ„Ž = 1)

Pressure loss in unsteady annular channel flow

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𝜚 = 0.01 𝜚 = 0.1 𝜚 = 0.5

Page 11: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

β€’ Influence of gap Womersley number π‘Šπ‘œβ„Ž on velocity profile (𝜚 = 0.5)

Pressure loss in unsteady annular channel flow

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π‘Šπ‘œβ„Ž = 1 π‘Šπ‘œβ„Ž = 10 π‘Šπ‘œβ„Ž = 100

Page 12: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Pressure loss in unsteady annular channel flow

β€’ Pressure loss can be derived based on velocity profile

β€’ Laplace transform of unsteady pressure loss:

Ξ”π‘βˆ—

Δ𝑧=πœ‚

π‘Ÿπ‘œ2 𝐹

βˆ— π‘Ÿπ‘œπ‘ 

𝜈, 𝜚 𝑒 βˆ—

πΉβˆ— =2

1 βˆ’ 𝜚2 𝐼0 πœšπ‘Ÿπ‘œπ‘ πœˆ 𝐾0 π‘Ÿπ‘œ

π‘ πœˆ βˆ’ 𝐼0 π‘Ÿπ‘œ

π‘ πœˆ 𝐾0 πœšπ‘Ÿπ‘œ

π‘ πœˆ π‘Ÿπ‘œ

π‘ πœˆ

𝐼1 π‘Ÿπ‘œπ‘ πœˆ βˆ’ 𝜚𝐼1 πœšπ‘Ÿπ‘œ

π‘ πœˆ 𝐾0 π‘Ÿπ‘œ

π‘ πœˆ βˆ’ 𝐾0 πœšπ‘Ÿπ‘œ

π‘ πœˆ + 𝐼0 π‘Ÿπ‘œ

π‘ πœˆ βˆ’ 𝐼0 πœšπ‘Ÿπ‘œ

π‘ πœˆ 𝐾1 π‘Ÿπ‘œ

π‘ πœˆ βˆ’ 𝜚𝐾1 πœšπ‘Ÿπ‘œ

π‘ πœˆ

βˆ’ 2

β€’ In oscillating flow, pressure loss depends on gap Womersley number and radius

ratio

β€’ For flows with arbitrary temporal distribution: derivation of inverse Laplace

transform of pressure loss formula

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Page 13: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Pressure loss in unsteady annular channel flow

β€’ Inverse Laplace transform of a product of two functions leads to a convolution

integral:

β„’βˆ’1 πΉβˆ—π‘’ βˆ— = 𝑒 𝑑1 𝐹 𝑑 βˆ’ 𝑑1

𝑑

0

d𝑑

β€’ Problem: There is no inverse Laplace transform of πΉβˆ—, since πΉβˆ— does not converge

to zero for 𝑠 β†’ ∞

β€’ Solution: Expansion with 𝑠/𝑠:

πΉβˆ—π‘’ βˆ— =πΉβˆ—

𝑠𝑠𝑒 βˆ— = π‘Šβˆ—π‘ π‘’ βˆ— = π‘Šβˆ—β„’

πœ•π‘’

πœ•π‘‘π‘ 

β€’ Inverse Laplace transform of π‘Šβˆ— can be derived by employing residue theorem

from complex analysis

β€’ Problems:

– Different inverse Laplace transform for every radius ratio 𝜚

– Determination of inverse Laplace transform cumbersome due to numerical

behaviour of Bessel functions

β€’ Solution?

β€’ For describing unsteady flows with arbitrary temporal distribution (e.g. water

hammer), the inverse Laplace transform of the pressure loss has to be derived.

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Page 14: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

1

2

3

4

Introduction to the problem of unsteady pressure loss

Pressure loss in unsteady annular channel flow

Summary & Outlook

Plane channel approximation

14

Outline

Page 15: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

β€’ Analysis of velocity profile: with decreasing channel height (𝜚 β†’ 1), the velocity

profile approaches that of a plane channel

β€’ Solution for small channel heights: replace actual problem of annular channel

flow with plane channel approximation

Plane channel approximation

15

πœ•π‘’

πœ•π‘‘+1

𝜌

πœ•π‘

πœ•π‘§= 𝜈

πœ•2𝑒

πœ•π‘Ÿ2+1

π‘Ÿ

πœ•π‘’

πœ•π‘Ÿ

πœ•π‘’

πœ•π‘‘+1

𝜌

πœ•π‘

πœ•π‘§= 𝜈

πœ•2𝑒

πœ•π‘¦2

Page 16: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Plane channel approximation

β€’ Approximated time domain expression for pressure loss in unsteady annular

channel flow: Δ𝑝

Δ𝑧=12πœ‚

β„Ž2𝑒 𝑑 +

πœ‚

β„Ž2 πœ•π‘’

πœ•π‘‘π‘‘1 π‘Šπ‘‘ 𝑑 βˆ’ 𝑑1

𝑑

0

d𝑑

β€’ For 𝑑 > 0.0023 β„Ž2/𝜈:

π‘Šπ‘‘ 𝑑𝑛 = 8 π‘’βˆ’80.76𝑑𝑛 + π‘’βˆ’238.72𝑑𝑛 + π‘’βˆ’475.59𝑑𝑛 + π‘’βˆ’791.43𝑑𝑛 +β‹―

β€’ For 𝑑 < 0.0023 β„Ž2/𝜈:

π‘Šπ‘‘ 𝑑𝑛 =2

πœ‹π‘‘π‘›βˆ’ 8 +

16

πœ‹π‘‘π‘› + 16𝑑𝑛 +

128

3 πœ‹π‘‘π‘›3 + 32𝑑𝑛

2 +β‹―

β€’ Error analysis: approximation error πœ€ less than 1% for radius ratios down

to 𝜚 = 0.5

β€’ Approximation suitable for most

practical purposes!

16

𝑑𝑛 =π‘‘πœˆ

β„Ž2

Page 17: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

1

2

3

4

Introduction to the problem of unsteady pressure loss

Pressure loss in unsteady annular channel flow

Summary & Outlook

Plane channel approximation

17

Outline

Page 18: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Summary & Outlook

β€’ Summary:

– The velocity profile for unsteady annular channel flow was derived

– Velocity profile depends on radius ratio & gap Womersley number

– Pressure loss depends on radius ratio & gap Womersley number

– Inverse Laplace transform of pressure loss formula is cumbersome due to

numerical behaviour of Bessel functions and variations in radius ratio

– For sufficiently narrow channels: plane channel approximation

– Approximation error of less than 1 % for radius ratios larger than 0.5

β€’ Outlook:

– Derivation of a curve fit of the approximated weighting function for efficient

simulation of transient events in annular channel flow

– Implementation into the simulation software DSHplus

– Expansion to shear flow (moving pipe wall or moving cylinder)

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Page 19: Pressure Loss in Unsteady Annular Channel Flow

Pasquini, Enrico

3/19/2018

Thank you for your attention!

Contact:

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β€’ Enrico Pasquini, M. Sc.

FLUIDON GmbH

Jülicher Straße 338a

52070 Aachen

[email protected]