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Simulation of a Geothermal System in COMSOL Multiphysics dokumenter/COMSOL... · Simulation of a...

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www.cmr.no © Christian Michelsen Research AS

Simulation of a Geothermal System in COMSOL Multiphysics

Knut-Erland Brun

Comsol Workshop 10/6/2011

www.cmr.no © Christian Michelsen Research AS

Outline

Background – geothermal energy

Comsol model

Geometry

Implementing physics

Meshing

Preliminary results

Outlook

3 Comsol Workshop 10/6/2011

www.cmr.no © Christian Michelsen Research AS

Geothermal energy

Geothermal Heat Pump

Comsol Workshop 10/6/2011 4

Illustration: Comfortbrygga.no

www.cmr.no © Christian Michelsen Research AS

Geothermal energy

Geothermal Heat Pump

Natural Geothermal Systems – e.g. Iceland

1-3 km – or less

Comsol Workshop 10/6/2011 5

www.cmr.no © Christian Michelsen Research AS

Geothermal energy

Geothermal Heat Pump

Natural Geothermal Systems – e.g. Iceland

1-3 km – or less

Enhanced Geothermal System («Hot Dry Rock»)

3-5 km – or more

Comsol Workshop 10/6/2011 6

Fracture-dominated porous media

• Earth-science module • Model fractures as internal boundaries

• BC: fluid flow along a fracture

www.cmr.no © Christian Michelsen Research AS

Geothermal energy

Geothermal Heat Pump

Natural Geothermal Systems – e.g. Iceland

1-3 km – or less

Enhanced Geothermal System («Hot Dry Rock»)

3-5 km – or more

Comsol Workshop 10/6/2011 7

Fracture-dominated porous media

• Earth-science module • Model fractures as internal boundaries

• BC: fluid flow along a fracture

www.cmr.no © Christian Michelsen Research AS

Geothermal energy

Geothermal Heat Pump

Natural Geothermal Systems – e.g. Iceland

1-3 km – or less

Enhanced Geothermal System («Hot Dry Rock»)

3-5 km – or more

Comsol Workshop 10/6/2011 8

Fracture-dominated porous media

• Jan’s work…

www.cmr.no © Christian Michelsen Research AS

Geothermal energy

Geothermal Heat Pump

Natural Geothermal Systems – e.g. Iceland

1-3 km – or less

Enhanced Geothermal System («Hot Dry Rock»)

3-5 km – or more

Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 9

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 10

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 11

Jan’s best tip:

• Parameterize everything! • Total control of all ‘parameters’; initial values, BC,

subdomain settings, etc. • Easy to make parametric sweeps

• Also geometric properties and mesh-values!

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 12

Jan’s best tip:

• Parameterize everything! • Total control of all ‘parameters’; initial values, BC,

subdomain settings, etc. • Easy to make parametric sweeps

• Also geometric properties and mesh-values!

www.cmr.no © Christian Michelsen Research AS

Wellbore Heat Exchanger – Physics/Geometry

Comsol Workshop 10/6/2011 13

Simple axial / single pipe

Axial symmetry

Flexible model: rwell : 0.10 - 0.15 m

rrock: 10 – 20 m

Depth 300 m – 5 km

www.cmr.no © Christian Michelsen Research AS

Wellbore Heat Exchanger – Physics/Geometry

Comsol Workshop 10/6/2011 14

Fluid inlet

Fluid outlet

www.cmr.no © Christian Michelsen Research AS

Wellbore Heat Exchanger – Physics/Geometry

Comsol Workshop 10/6/2011 15

d

rrock

rwell

Fluid inlet

Fluid outlet

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Heat transfer by forced convection

• 𝜙𝑇 = ℎ𝐴(𝑇ℎ − 𝑇𝑙)

• 𝑇ℎ − rock temperature

• 𝑇𝑙 − fluid temperature

Heat transfer by conduction

• 𝜙𝑇 = 𝑘𝑇𝛻𝑇

Comsol Workshop 10/6/2011 16

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Heat transfer by forced convection

• 𝜙𝑇 = ℎ𝐴(𝑇ℎ − 𝑇𝑙)

• 𝑇ℎ − rock temperature

• 𝑇𝑙 − fluid temperature

Heat transfer by conduction

• 𝜙𝑇 = 𝑘𝑇𝛻𝑇

Comsol Workshop 10/6/2011 17

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Heat transfer by forced convection

• 𝜙𝑇 = ℎ𝐴(𝑇ℎ − 𝑇𝑙)

• 𝑇ℎ − rock temperature

• 𝑇𝑙 − fluid temperature

Heat transfer by conduction

• 𝜙𝑇 = 𝑘𝑇𝛻𝑇

Comsol Workshop 10/6/2011 18

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 19

Heat transfer by forced convection

• Continuity or ‘Thin thermally resistive layer’?

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 20

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 21

Mesh

• Difficult geometry: • Long, thin pipe • Need small, high-quality elements in the pipe • Need large elements in rock to reduce

computation time

• Implement a mesh-refinement parameter

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 22

Mesh

• Difficult geometry: • Long, thin pipe • Need small, high-quality elements in the pipe • Need large elements in rock to reduce

computation time

• Implement a mesh-refinement parameter

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 23

Mesh

• Difficult geometry: • Long, thin pipe • Need small, high-quality elements in the pipe • Need large elements in rock to reduce

computation time

• Implement a mesh-refinement parameter

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 24

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 25

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 26

www.cmr.no © Christian Michelsen Research AS

Comsol Model of a Wellbore Heat Exchanger

Comsol Workshop 10/6/2011 27

www.cmr.no © Christian Michelsen Research AS

Preliminary results

Comsol Workshop 10/6/2011 28

The effect of a thin thermally resistive layer

www.cmr.no © Christian Michelsen Research AS

Preliminary results

Comsol Workshop 10/6/2011 29

Cut-line plot

Continuity of temperature. The ‘jump’ in the rock temperature observed about

r=0.45 m is assumed due to interpolation of the solution using 2nd-degree

polynomials.

www.cmr.no © Christian Michelsen Research AS

Preliminary results

Comsol Workshop 10/6/2011 30

Table plot

Outflow temperature after 200 days. Observe the small difference this layer

makes; it can be quantified to less than 0.1 ˚C

www.cmr.no © Christian Michelsen Research AS

Outlook – further work

Study behavior for three cases – both fluid and rock temperature

500 m well

1 km well

5 km well

Imitate the behavior of a U-pipe by mirroring the model at z=-d (total

depth = 2d)

Future model: Coaxial

Comsol Workshop 10/6/2011 31


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