IP Library › Granted Patent US 7,643,977

Granted Patent B2

US 7,643,977 · App. 11/468,118 · Granted Jan 5, 2010

System and method for predicting performance of electrical power cables

View Patent ↗

Loading inventors, assignments & file history…

Monitor This Case

Get email alerts when status or documents change.

Order Certified Copies

Most orders are placed with the USPTO same day — all within 24 business hours.

Order via The Patent Place →

Pre-filled with this patent's details

Quick Facts

Patent No.: US 7,643,977
App. No.: 11/468,118
Granted: Jan 5, 2010
Kind: B2

External Links

USPTO Patent Center↗ Full Patent PDF↗

Abstract

A computer simulation method is disclosed for simulating an electrical cable having a stranded conductor surrounded by a conductor shield encased in an insulation jacket and having an interstitial void volume in the region of the conductor injected with a fluid composition comprising at least one dielectric enhancement fluid component so as to at least partially fill the interstitial void volume at an initial time. The simulation method comprises for a selected length of the simulated cable, defining a plurality of radially arranged finite volumes extending the selected length of the simulated cable, and estimating the radial temperature of each finite volume. For a selected time period after the initial time, performing a series of steps at least once and outputting or otherwise using the value of the new concentration for the dielectric enhancement fluid component within each finite volume.

Claims (117)

1. A computer simulation method for simulating an electrical cable having a stranded conductor surrounded by a conductor shield encased in an insulation jacket and having an interstitial void volume in the region of the conductor injected with a fluid composition comprising at least one dielectric enhancement fluid component so as to at least partially fill the interstitial void volume at an initial time t=0, the simulation method comprising: for a selected length of the simulated cable, defining a plurality of radially arranged finite volumes extending the selected length of the simulated cable; for each of a plurality of different selected incremental time periods occurring after t=0: estimating the radial temperature of each finite volume; calculating the change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions using the estimated radial temperature; calculating the diffusion properties of the dielectric enhancement fluid component within each finite volume using the estimated radial temperature; calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid component within the finite volumes; and combining the calculated change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions with the calculated mass flux between each adjacent finite volume for the dielectric enhancement fluid component within the finite volumes to determine a new concentration for the dielectric enhancement fluid component within each finite volume; and outputting the value of the new concentration for the dielectric enhancement fluid component within each finite volume.

2. The computer simulation method of claim 1 , further including using the outputted value of the new concentration for the dielectric enhancement fluid component within each finite volume to determine a calculated concentration profile for the dielectric enhancement fluid component within the conductor shield and the insulation jacket of the simulated cable for at least one time after t=0, and using the calculated concentration profile to select a suitable fluid composition for injection into the electrical cable being simulated.

3. The computer simulation method of claim 2 , further including providing an empirical model of the dielectric performance of the simulated cable as a function of concentration of the dielectric enhancement fluid component, and using the empirical model and the calculated concentration profile for the dielectric enhancement fluid component within the conductor shield and the insulation jacket of the simulated cable to determine an estimate of dielectric performance changes for at least one time after t=0.

4. The computer simulation method of claim 1 wherein the finite volumes are a plurality of coaxial cylinders extending the selected length of the simulated cable.

5. The computer simulation method of claim 1 , further including:

using the outputted value of the new concentration for the dielectric enhancement fluid component within each finite volume to determine a first calculated concentration profile for the dielectric enhancement fluid component within the conductor shield and the insulation jacket of the simulated cable for a selected time after t=0;

for each of a plurality of different selected incremental time periods occurring after t=0 using a selected constant radial temperature for each finite volume:

calculating the change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid component within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid component within the finite volumes; and

combining the calculated change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions with the calculated mass flux between each adjacent finite volume for the dielectric enhancement fluid component within the finite volumes to determine a new concentration for the dielectric enhancement fluid component within each finite volume;

outputting the value of the new concentration for the dielectric enhancement fluid component within each finite volume using the selected constant radial temperature;

using the outputted value of the new concentration for the dielectric enhancement fluid component within each finite volume using the selected constant radial temperature to determine a second calculated concentration profile for the dielectric enhancement fluid component within the conductor shield and the insulation jacket of the simulated cable for the selected time after t=0;

determining if the second calculated concentration profile approximates the first calculated concentration profile; and

using the selected constant radial temperature as a flux-weighted temperature if the second calculated concentration profile approximates the first calculated concentration profile.

6. The computer simulation method of claim 5 , wherein if the second calculated concentration profile does not approximate the first calculated concentration profile, selecting a different constant radial temperature for each finite volume to use for each of the plurality of different selected incremental time periods occurring after t=0, until the second calculated concentration profile approximates the first calculated concentration profile.

7. The computer simulation method of claim 5 wherein the flux-weighted temperature is used to select a suitable fluid composition for injection into the electrical cable being simulated.

8. The computer simulation method of claim 1 , further including:

determining a constant radial temperature for each finite volume that results in a second calculated concentration profile for the dielectric enhancement fluid component within the conductor shield and the insulation jacket of the simulated cable for the selected time after t=0 that approximates the first calculated concentration profile, by:

selecting a constant radial temperature for each finite volume to use in determining the second calculated concentration profile;

using the selected constant radial temperature, for each of a plurality of different selected incremental time periods occurring after t=0:

calculating the change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid component within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid component within the finite volumes;

outputting the value of the new concentration for the dielectric enhancement fluid component within each finite volume using the selected constant radial temperature;

determining if the second calculated concentration profile approximates the first calculated concentration profile;

if the selected constant radial temperature does not result in the second calculated concentration profile being determined to approximate the first calculated concentration profile, selecting a new constant radial temperature to use in determining the second calculated concentration profile; and

if the selected constant radial temperature does result in the second calculated concentration profile being determined to approximate the first calculated concentration profile, using the selected constant radial temperature as a flux-weighted temperature.

9. A computer simulation method for simulating an electrical cable having a stranded conductor surrounded by a conductor shield encased in an insulation jacket and having an interstitial void volume in the region of the conductor injected with a fluid composition comprising at least one dielectric enhancement fluid component so as to at least partially fill the interstitial void volume at an initial time, the simulation method comprising: for a selected length of the simulated cable, defining a plurality of radially arranged finite volumes extending the selected length of the simulated cable; estimating the radial temperature of each finite volume; for a selected time period after the initial time, performing at least once each of: calculating the change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions using the estimated radial temperature; calculating the diffusion properties of the dielectric enhancement fluid component within each finite volume using the estimated radial temperature; calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid component within the finite volumes; and combining the calculated change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions with the calculated mass flux between each adjacent finite volume for the dielectric enhancement fluid component within the finite volumes to determine a new concentration for the dielectric enhancement fluid component within each finite volume; and outputting the value of the new concentration for the dielectric enhancement fluid component within each finite volume.

10. The computer simulation method of claim 9 , further including:

determining a constant radial temperature for each finite volume that results in a second calculated concentration profile for the dielectric enhancement fluid component within the conductor shield and the insulation jacket of the simulated cable for the selected time period after the initial time that approximates the first calculated concentration profile, by:

selecting a constant radial temperature for each finite volume to use in determining the second calculated concentration profile;

using the selected constant radial temperature, for a selected time period after the initial time, performing at least once each of:

calculating the change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid component within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid component within the finite volumes;

outputting the value of the new concentration for the dielectric enhancement fluid component within each finite volume using the selected constant radial temperature;

determining if the second calculated concentration profile approximates the first calculated concentration profile;

11. The computer simulation method of claim 10 wherein the flux-weighted temperature is used to select a suitable fluid composition for injection into the electrical cable being simulated.

12. A computer simulation method for simulating an electrical cable having a stranded conductor surrounded by a conductor shield encased in an insulation jacket and having an interstitial void volume in the region of the conductor injected with a fluid composition comprising at least one dielectric enhancement fluid component so as to at least partially fill the interstitial void volume at an initial time, the simulation method comprising:

for a selected length of the simulated cable, defining a plurality of radially arranged finite volumes extending the selected length of the simulated cable;

estimating the radial temperature of each finite volume;

for a selected time period after the initial time, performing at least once each of:

calculating the change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid component within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid component within the finite volumes; and

using the new concentration for the dielectric enhancement fluid component within each finite volume to determine a calculated concentration profile for the dielectric enhancement fluid component within the conductor shield and the insulation jacket of the simulated cable for the selected time period after the initial time; and

using the calculated concentration profile to select a suitable fluid composition for injection into the electrical cable being simulated.

13. The computer simulation method of claim 12 , further including providing an empirical model of the dielectric performance of the simulated cable as a function of concentration of the dielectric enhancement fluid component, and using the empirical model and the calculated concentration profile for the dielectric enhancement fluid component within the conductor shield and the insulation jacket of the simulated cable to determine an estimate of dielectric performance changes for times after the initial time.

14. A computer simulation method for simulating an electrical cable having a stranded conductor surrounded by a conductor shield encased in an insulation jacket and having an interstitial void volume in the region of the conductor injected with a fluid composition comprising a plurality of dielectric enhancement fluid components so as to at least partially fill the interstitial void volume at an initial time t=0, the simulation method comprising:

for a selected length of the simulated cable, defining a plurality of radially arranged finite volumes extending the selected length of the simulated cable;

estimating the radial temperature of each finite volume;

for each of a plurality of different selected incremental time periods occurring after t=0:

calculating the changes in mass of the dielectric enhancement fluid components within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid components within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid components within the finite volumes; and

combining the calculated change in mass of the dielectric enhancement fluid components within each finite volume due to chemical reactions with the calculated mass flux between each adjacent finite volume for the dielectric enhancement fluid components within the finite volumes to determine new concentrations for the dielectric enhancement fluid components within each finite volume; and

outputting the values of the new concentrations for the dielectric enhancement fluid components within each finite volume.

15. The computer simulation method of claim 14 , further including:

using the outputted values of the new concentrations for the dielectric enhancement fluid components within each finite volume to determine a first combined calculated concentration profile for the dielectric enhancement fluid components within the conductor shield and the insulation jacket of the simulated cable for a selected time after t=0;

determining a constant radial temperature for each finite volume that results in a second combined calculated concentration profile for the dielectric enhancement fluid components within the conductor shield and the insulation jacket of the simulated cable for the selected time after t=0 that approximates the first calculated concentration profile, by:

selecting a constant radial temperature for each finite volume to use in determining the second combined calculated concentration profile;

using the selected constant radial temperature, for each of a plurality of different selected incremental time periods occurring after t=0:

calculating the change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid component within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid component within the finite volumes;

combining the calculated change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions with the calculated mass flux between each adjacent finite volume for the dielectric enhancement fluid components within the finite volumes to determine a new concentration for the dielectric enhancement fluid component within each finite volume;

outputting the values of the new concentrations for the dielectric enhancement fluid components within each finite volume using the selected constant radial temperature;

using the outputted values of the new concentrations for the dielectric enhancement fluid components within each finite volume using the selected constant radial temperature to determine the second combined calculated concentration profile;

determining if the second combined calculated concentration profile approximates the first combined calculated concentration profile;

if the selected constant radial temperature does not result in the second combined calculated concentration profile being determined to approximate the first combined calculated concentration profile, selecting a new constant radial temperature to use in determining the second combined calculated concentration profile; and

if the selected constant radial temperature does result in the second combined calculated concentration profile being determined to approximate the first combined calculated concentration profile, using the selected constant radial temperature as a flux-weighted temperature.

16. A computer simulation method for simulating an electrical cable having a stranded conductor surrounded by a conductor shield encased in an insulation jacket and having an interstitial void volume in the region of the conductor injected with a fluid composition comprising a plurality of dielectric enhancement fluid components so as to at least partially fill the interstitial void volume at an initial time t=0, the simulation method comprising:

for a selected length of the simulated cable, defining a plurality of radially arranged finite volumes extending the selected length of the simulated cable;

estimating the radial temperature of each finite volume;

for each of a plurality of different selected incremental time periods occurring after t=0:

calculating the changes in mass of the dielectric enhancement fluid components within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid components within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid components within the finite volumes; and

using the new concentrations for the dielectric enhancement fluid components within each finite volume to determine a calculated concentration profile for each of the dielectric enhancement fluid components within the conductor shield and the insulation jacket of the simulated cable for at least one time after t=0; and

using the calculated concentration profile for each of the dielectric enhancement fluid components to select a suitable fluid composition for injection into the electrical cable being simulated.

17. The computer simulation method of claim 16 , further including providing an empirical model of the dielectric performance of the simulated cable as a function of concentrations of the dielectric enhancement fluid components, and using the empirical model and the calculated concentration profiles for the dielectric enhancement fluid components within the conductor shield and the insulation jacket of the simulated cable to determine an estimate of dielectric performance changes for times after the initial time.

18. A computer simulation method for simulating an electrical cable having a stranded conductor surrounded by a conductor shield encased in an insulation jacket and having an interstitial void volume in the region of the conductor injected with a fluid composition comprising a plurality of dielectric enhancement fluid components so as to at least partially fill the interstitial void volume at an initial time, the simulation method comprising:

for a selected length of the simulated cable, defining a plurality of radially arranged finite volumes extending the selected length of the simulated cable;

estimating the radial temperature of each finite volume;

for a selected time period after the initial time, performing at least once for each of the dielectric enhancement fluid components, each of:

calculating the changes in mass of the dielectric enhancement fluid components within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid components within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid components within the finite volumes; and

outputting the values of the new concentrations for the dielectric enhancement fluid components within each finite volume.

19. The computer simulation method of claim 18 , further including using the outputted values of the new concentrations for the dielectric enhancement fluid components within each finite volume to determine for each of the dielectric enhancement fluid components a calculated concentration profile within the conductor shield and the insulation jacket of the simulated cable for the selected time period after the initial time, and using the calculated concentration profiles to select a suitable fluid composition for injection into the electrical cable being simulated.

20. The computer simulation method of claim 19 , further including providing an empirical model of the dielectric performance of the simulated cable as a function of concentrations of the dielectric enhancement fluid components, and using the empirical model and the calculated concentration profiles for the dielectric enhancement fluid components within the conductor shield and the insulation jacket of the simulated cable to determine an estimate of dielectric performance changes for times after the initial time.

21. The computer simulation method of claim 18 , further including:

determining a constant radial temperature for each finite volume that results in a second combined calculated concentration profile for the dielectric enhancement fluid components within the conductor shield and the insulation jacket of the simulated cable for the selected time period after the initial time that approximates the first combined calculated concentration profile, by:

selecting a constant radial temperature for each finite volume to use in determining the second combined calculated concentration profile;

using the selected constant radial temperature, for the selected time period after the initial time:

calculating the change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions;

calculating the diffusion properties of the dielectric enhancement fluid component within each finite volume;

calculating the mass flux from one finite volume to another finite volume for the dielectric enhancement fluid component within the finite volumes;

combining the calculated change in mass of the dielectric enhancement fluid component within each finite volume due to chemical reactions with the calculated mass flux between each adjacent finite volume for the dielectric enhancement fluid components within the finite volumes to determine a new concentration for the dielectric enhancement fluid component within each finite volume;

outputting the values of the new concentrations for the dielectric enhancement fluid components within each finite volume using the selected constant radial temperature;

determining if the second combined calculated concentration profile approximates the first combined calculated concentration profile;

Assignments (7)

RELEASE OF SECURITY INTEREST Recorded Jul 31, 2025

From: WELLS FARGO BANK, NATIONAL ASSOCIATION

To: SOUTHWIRE COMPANY, LLC; COLEMAN CABLE, LLC; TECHNOLOGY RESEARCH, LLC; SUMNER MANUFACTURING COMPANY, LLC; MADISON ELECTRIC PRODUCTS, LLC; NOVINIUM, LLC; NOVINIUM HOLDINGS, INC.; WATTEREDGE, LLC; TAPPAN WIRE & CABLE, LLC; UNITED COPPER INDUSTRIES, LLC; TOPAZ LIGHTING COMPANY LLC; OBI PARTNERS, LLC; WIIP, INC.

Reel/Frame 072299/0141 →

TERMINATION AND RELEASE OF INTELLECTUAL PROPERTY SECURITY AGREEMENTS Recorded Oct 23, 2024

From: BANK OF AMERICA, N.A., AS AGENT

To: SOUTHWIRE COMPANY, LLC; COLEMAN CABLE, LLC (F/K/A COLEMAN CABLE, INC.); TECHNOLOGY RESEARCH, LLC (F/K/A TECHNOLOGY RESEARCH CORPORATION); SUMNER MANUFACTURING COMPANY, LLC; MADISON ELECTRIC PRODUCTS, LLC; NOVINIUM, LLC; WATTEREDGE, LLC; TAPPAN WIRE & CABLE, LLC; UNITED COPPER INDUSTRIES, LLC; TOPAZ LIGHTING COMPANY LLC; OBI PARTNERS, LLC; WIIP, INC.

Reel/Frame 069235/0104 →

AMENDMENT NO. 5 TO GRANT OF SECURITY INTEREST IN PATENT RIGHTS Recorded Jun 13, 2022

From: SOUTHWIRE COMPANY, LLC; SUMNER MANUFACTURING COMPANY, LLC; COLEMAN CABLE, LLC; TECHNOLOGY RESEARCH, LLC; MADISON ELECTRIC PRODUCTS LLC; NOVINIUM, LLC

To: BANK OF AMERICA, N.A., AS COLLATERAL AGENT

Reel/Frame 060345/0048 →

AMENDMENT NO. 5 TO GRANT OF SECURITY INTERESTS IN PATENT RIGHTS Recorded Jun 13, 2022

From: NOVINIUM HOLDINGS, INC.; NOVINIUM, LLC

To: WELLS FARGO BANK, NATIONAL ASSOCIATION

Reel/Frame 060345/0058 →

CHANGE OF NAME Recorded May 4, 2022

From: NOVINIUM, INC.

To: NOVINIUM, LLC

Reel/Frame 059854/0073 →

SECURITY INTEREST Recorded Aug 26, 2020

From: NOVINIUM, INC.; UTILX CORPORATION; UTILX OVERSEAS HOLDINGS, INC.; PLENOVO, INC.

To: STAR MOUNTAIN DIVERSIFIED CREDIT INCOME FUND III, L.P.

Reel/Frame 053609/0185 →

RELEASE OF SECURITY INTEREST Recorded Aug 17, 2020

From: MIDCAP FINANCIAL TRUST

To: UTILX CORPORATION; NOVINIUM, INC.

Reel/Frame 053509/0223 →