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Dive into the research topics where M. J. Gouge is active.

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Featured researches published by M. J. Gouge.


IEEE Transactions on Applied Superconductivity | 2003

Measurements of temperature dependence of the stability and quench propagation of a 20-cm-long RABiTS Y-Ba-Cu-O tape

Robert Grabovickic; J. W. Lue; M. J. Gouge; J. A. Demko; R. C. Duckworth

Thermal stability and quench propagation in a composite tape made of YBa/sub 2/Cu/sub 3/O/sub x/ (YBCO) superconductor were studied experimentally. Quench propagation in each test was initiated by applying a sequence of a short overcurrent pulse followed by a longer pulse at a typical operating current for the tape. The resulting change in resistivity due to internal heating was measured through voltage taps across different zones of the tape. Measurements were performed as a function of both initial overcurrent and operating current for several operating temperatures between 45 and 80 K. These experimental results provided the thermal stability margin, the minimum propagation current, and the quench propagation velocity for the tape. Experimentally obtained temperature dependence of normal zone propagation velocity was compared with the adiabatic theory taking into account minimum propagation current. It was noted that the measured normal zone propagation velocity compared favorably with the theory at each operating temperature.


IEEE Transactions on Applied Superconductivity | 2001

Installation and operation of the Southwire 30-meter high-temperature superconducting power cable

J.P. Stovall; J. A. Demko; P.W. Fisher; M. J. Gouge; J. W. Lue; U. Sinha; J.W. Armstrong; R. L. Hughey; D. Lindsay; Jerry C. Tolbert

Southwire Company has installed, tested and is operating the first real-world application of a high-temperature superconducting cable system at its headquarters in Carrollton, GA, USA. The cable is powering three Southwire manufacturing plants, marking the first time a company has successfully made the difficult transition front laboratory to practical field application of an HTS cable. The cables are rated at 12.4-kV, 1250-A, 60 Hz and are cooled with pressurized liquid nitrogen at temperatures from 70-80 K. Before placing the cables into service, extensive offline electrical testing was performed including voltage withstand, measurement of DC critical current, extended load current testing, rated voltage testing and partial discharge measurement. The cables were energized on Jan. 5, 2000 for online testing and operation, and by the end of August 2000, had provided 100% of the customer load for 2164 hours.


IEEE Transactions on Applied Superconductivity | 2007

Triaxial HTS Cable for the AEP Bixby Project

J. A. Demko; I. Sauers; D. R. James; M. J. Gouge; D. Lindsay; Mark Roden; Jerry C. Tolbert; Dag Willén; C.T. Nielsen

Ultera has installed a single 200-meter long high temperature superconducting (HTS) 3-phase triaxial design cable at the American electric power (AEP) Bixby substation in Columbus, Ohio. The cable connects a 138/13.2 kV transformer to the distribution switchgear serving seven outgoing circuits. It was designed to carry 3000 Arms. Testing of 3- to 5-meter length prototype cables, including a 5-meter prototype with full scale terminations tested at ORNL was conducted prior to the manufacture and installation of the AEP triaxial cable. These prototypes were used to demonstrate the crucial operating conditions including steady state operation at the 3000 Arms design current, high voltage operation, high voltage withstand and 110 kV impulse, and overcurrent fault capability. A summary of the results from the thermal analysis and testing conducted by Ultera and ORNL will be presented. Some analysis of the cable thermal-hydraulic response based on the testing that were used to determine some of the cable cryogenic system requirements are also presented.


IEEE Transactions on Applied Superconductivity | 2005

Tests of tri-axial HTS cables

M. J. Gouge; D. Lindsay; J. A. Demko; R. C. Duckworth; Alvin R Ellis; P.W. Fisher; D. R. James; J. W. Lue; Mark Roden; I. Sauers; Jerry C. Tolbert; Chresten Træholt; Dag Willén

The Ultera/ORNL team have built and tested 3-m and 5-m triaxial cables rated at 3 and 1.3 kA-rms, respectively. The three concentric superconducting phases are made of BSCCO-2223 HTS tapes, separated by layers of cold-dielectric tapes. A copper braid is added as the grounding shield on the outside of the three active phases. Tests of these cables were performed at temperatures ranging from 70 to 84 K. AC loss data reconfirmed the previous result on a 1.5-m prototype cable that the total 3-phase ac loss is about the sum of the calculated ac losses of the three concentric phases. These and other test results of the 1.3 and 3 kA cables will be used to construct a second 5-m triaxial cable rated at 3 kA-rms, 15 kV. Preliminary test results supporting this new cable and the associated termination are summarized.


IEEE Transactions on Applied Superconductivity | 2005

Feasibility of electric power transmission by DC superconducting cables

Pritindra Chowdhuri; Chandralekha Pallem; J. A. Demko; M. J. Gouge

The electrical characteristics of dc superconducting cables of two power ratings were studied: 3 GW and 500 MW. Two designs were considered for each of the two power ratings. In the first design, the SUPPLY stream of the cryogen is surrounded by the high-voltage high-temperature superconductor cylinder. The RETURN stream of the cryogen is on the grounded side of the system. In the second design, both the SUPPLY and the RETURN streams of the cryogen are on the grounded side of the cable. Two electrical characteristics of these cables were studied: 1) fault currents and 2) current harmonics. It was concluded that neither the fault currents nor the current harmonics pose any problems in the operation of the dc superconducting cables.


IEEE Transactions on Applied Superconductivity | 2005

Substrate and stabilization effects on the transport AC losses in YBCO coated conductors

R. C. Duckworth; M. J. Gouge; J. W. Lue; C.L.H. Thieme; D.T. Verebelyi

In support of second generation HTS conductor development for ac applications, transport ac loss measurements were conducted on a series of RABiTS-processed YBa/sub 2/Cu/sub 3/O/sub x/ (YBCO) coated conductors with different nickel alloy substrates and copper stabilization at 77 K. Each 1-cm wide sample had a critical current density between 1.0 and 2.0 MA/cm/sup 2/ and had either a 75 /spl mu/m Ni-5at%W substrate or a 75 /spl mu/m Ni-10%Cr-2%W substrate with 2-/spl mu/m nickel overlayer. Samples with copper stabilization had a 50-/spl mu/m strip of 1 cm wide copper laminated to a 3-/spl mu/m thick silver coated YBCO sample. Using thermal and electrical measurement techniques, the ac losses were measured as a function of the peak current ratio at 60 Hz. Experimental results were compared to the Norris thin strip and elliptical models to determine the influence of the ferromagnetic loss of the substrate and the copper lamination on the total ac loss.


IEEE Transactions on Applied Superconductivity | 2003

Measurements of the performance of BSCCO HTS tape under magnetic fields with a cryocooled test rig

M. A. Young; J. A. Demko; M. J. Gouge; M.O. Pace; J. W. Lue; Robert Grabovickic

The use of high-temperature superconducting (HTS) materials for electric power applications is being realized in prototype systems. A test rig was designed and fabricated that uses a 6-T cryocooled magnet with an 20.3 cm warm bore. Inserted in the bore is a stainless steel vacuum vessel that has a Cryomech GB37 cryocooler to conductively cool the sample. Critical current measurements were made on BSCCO-2223 tapes under externally applied perpendicular and parallel magnetic fields. A description of the test rig design and results from a series of measurements will be presented.


IEEE Transactions on Applied Superconductivity | 2003

The role of nickel substrates in the quench dynamics of silver coated YBCO tapes

Robert C. Duckworth; J. W. Lue; D.F. Lee; Robert Grabovickic; M. J. Gouge

A pair of silver coated YBCO tapes with varying degrees of electrical contact between the silver and the YBCO nickel substrate were studied to examine the impact of nickel on normal zone formation and stability. The YBCO tapes were fabricated using the rolling assisted bi-axially textured (RABiTS) method and 15-cm-long samples with 2 /spl mu/m of silver were prepared. The samples were place in a conduction cooling environment at 45 K to study quench or recovery when a series of dc transient over-current pulses were applied. We used a series of voltage taps on both the silver and nickel to characterize the nature of the contact between the silver and the nickel through the measured voltages. In as-manufactured samples and those sample with continuous contact between the nickel and silver, we found that the silver and nickel can not be treated as conductors in parallel when a normal zone is present because of current present in the nickel even while sections of the sample remains superconducting. This nonparallel contact makes stability characterization difficult although the samples with intentional contact were able to withstand larger current pulses. In addition, the samples with intentional electrical contact between the silver and nickel exhibited normal zone propagation in both the silver and the nickel with speeds between 4 mm/s and 8 mm/s.


IEEE Transactions on Applied Superconductivity | 2001

Practical AC loss and thermal considerations for HTS power transmission cable systems

J. A. Demko; J. W. Lue; M. J. Gouge; J.P. Stovall; Z. Butterworth; U. Sinha; R. L. Hughey

The use of high-temperature superconducting materials for power-transmission cable applications is being realized in prototype situations. It is well known that AC loss decreases as the temperature of the conductor decreases. Also, thermal losses are higher at lower temperatures, owing to the increased temperature difference between ambient and cryogenic operating conditions. Both counterflow and parallel-flow cooling arrangements have been proposed in the literature and significantly affect temperature distribution along the cable. In this investigation, the counteracting AC loss and thermal losses are analyzed for both cooling configurations to determine the benefits and limits of each. The thermal-insulation performance levels of materials versus those of typical systems in operation are presented. Widespread application of long-length flexible cable systems, from the refrigeration point of view, will depend on an energy-efficient cryogenic system that is economical to manufacture and operate. While the counterflow arrangement will typically have a lower heat load, it has a length limit arising from the large pressure drop associated with the configuration.


IEEE Transactions on Applied Superconductivity | 2005

Over-current testing of HTS tapes

J. W. Lue; M. J. Gouge; R. C. Duckworth

High-temperature superconducting (HTS) transmission cables are subjected to short-circuit fault currents 10 to 30 times the normal operating current and lasting up to 15 cycles. These over-currents will drive the HTS conductor normal and generate heat during the fault. A concern is whether the fault current will either electromechanically or thermally damage the HTS conductor and degrade it or burn-out the tape altogether. Electromechanical and thermal limitations of over-current pulses were measured on BSCCO and YBCO tapes in a liquid nitrogen bath. With pulse lengths as short as 35 ms, it is found that single BSCCO and YBCO tapes can be pulsed to at least 1 to 1.2 kA without being damaged electromechanically. Longer pulses at moderate (450-750 A) over-currents indicated that HTS tapes can be heated transiently to over 400 K without suffering degradation. Thus, it is likely that other considerations of the cable rather than the HTS tape itself would set the limit for short-circuit fault protection.

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J. A. Demko

Oak Ridge National Laboratory

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J. W. Lue

Oak Ridge National Laboratory

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P.W. Fisher

Oak Ridge National Laboratory

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R. C. Duckworth

Oak Ridge National Laboratory

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D. Lindsay

Oak Ridge National Laboratory

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S. L. Milora

Oak Ridge National Laboratory

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S.K. Combs

Oak Ridge National Laboratory

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C.R. Foust

Oak Ridge National Laboratory

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J.P. Stovall

Oak Ridge National Laboratory

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L. R. Baylor

Oak Ridge National Laboratory

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