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Articles

A finite line source simulation model for geothermal systems with series- and parallel-connected boreholes and independent fluid loops

Pages 414-432 | Received 23 Jun 2017, Accepted 13 Sep 2017, Published online: 20 Oct 2017
 

Abstract

A model for the simulation of geothermal systems with parallel- and series-connected boreholes is presented. Mass and heat balance problems are formulated for each component in the system and are assembled into system-level problems. A third problem is formulated to account for heat transfer in the bore field, using the finite line source solution. This third problem is coupled to the system-level heat balance problem by an analytical solution of the heat transfer inside boreholes with multiple U-tubes. The simulation model allows for any number of independent fluid loops within the bore field or within individual boreholes and allows for combinations of specified inlet fluid temperatures and heat extraction rates in independent fluid loops. The model accounts for the axial variation of the fluid and borehole wall temperatures and heat extraction rates. The capabilities of the model are demonstrated through three example simulations.

Nomenclature

Variables

αs=

Soil thermal diffusivity

Δt=

Simulation time step

Δtp=

Size of aggregation cell p

ΔTb=

Borehole wall temperature drop

cp=

Specific heat capacity

COP=

Heat pump coefficient of performance

d=

Distance between boreholes

D=

Borehole or borehole segment buried depth

=

Absolute error tolerance on borehole wall temperatures

=

Absolute error tolerance on fluid temperatures

=

Relative error tolerance on fluid mass flow rates

G=

Captured solar radiation

h=

Segment-to-segment thermal response factor

H=

Borehole or borehole segment length

ks=

Ground thermal conductivity

=

Inlet fluid mass flow rate

=

Outlet fluid mass flow rate

η=

Solar collector efficiency

Nagg=

Total number of load aggregation cells

Nb=

Total number of boreholes in bore field

Nc=

Total number of system components

nin=

Number of inlets in component

Nin=

Total number of inlets in system

nout=

Number of outlets in component

Nout=

Total number of outlets in system

np=

Number of U-tubes in borehole

Np=

Total number of U-tubes in bore field

nq=

Number of borehole segments in borehole

Nq=

Total number of borehole segments in bore field

=

Component heat transfer rate

=

Borehole heat extraction rate

=

Building load

=

Pipe heat transfer rate

=

Borehole radius

=

Delta-circuit thermal resistance

=

Effective borehole thermal resistance

=

Fluid to outer pipe wall thermal resistance

=

Pipe inner radius

=

Pipe outer radius

t=

Time

Ta=

Ambient temperature

Tb=

Borehole wall temperature

Tf=

Fluid temperature in borehole pipes

Tf,in=

Inlet fluid temperature

Tf,out=

Outlet fluid temperature

Tg=

Undisturbed ground temperature

(x,y)=

Coordinates of boreholes or pipes

z=

Depth

Matrices and vectors

A=

Coefficient matrix of the system of differential equations for fluid temperatures in boreholes

=

Coefficient matrix for the component-level mass balance problem

=

Coefficient matrix for the system-level mass balance problem

=

Coefficient matrix for the borehole heat transfer problem

=

Coefficient matrix for the bore field heat transfer problem

=

Coefficient matrix for the component-level heat balance problem

=

Coefficient matrix for the system-level heat balance problem

=

Coefficient vector for the component-level mass balance problem

=

Coefficient vector for the system-level mass balance problem

=

Coefficient vector for the borehole heat transfer problem

=

Coefficient vector for the bore field heat transfer problem

=

Coefficient vector for the component-level heat balance problem

=

Coefficient vector for the system-level heat balance problem

C=

Component connectivity matrix

E=

Matrix exponential of Az

Ein, Eout, Eb=

Coefficient matrices for boundary condition at z = H

H=

Matrix of segment-to-segment thermal response factors

I=

Identity matrix

L=

Diagonal matrix of eigenvalues of A

=

Vector of inlet fluid mass flow rates

=

Vector of outlet fluid mass flow rates

=

Vector of heat extraction rate per unit length of borehole segments

Tb=

Vector of average borehole segment temperatures

Tb,0=

Vector of average borehole segment temperatures assuming no heat extraction during current time step

Tf,in=

Vector of inlet fluid temperatures

Tf,out=

Vector of outlet fluid temperatures

Tf=

Vector of fluid temperatures in borehole pipes

Tg=

Vector of undisturbed ground temperatures

V=

Matrix of eigenvectors of A

y=

Vector of mass flow rate fractions

Indices

ib, jb=

Borehole indices

ic, jc=

Component indices

ip, jp=

Pipe indices

k=

Time index

specified=

Specified value of the variable

tot=

Total value in the bore field

u,v=

Borehole segment indices

Additional information

Funding

The author received a start-up subsidy from the Fonds de Recherche du Québec – Nature et Technologies (FRQNT) [2015-B3-181989].
This article is part of the following collections:
Journal of Building Performance Simulation Best Paper Award

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