diff options
author | Angelo Rossi <angelo.rossi.homelab@gmail.com> | 2023-06-21 12:04:16 +0000 |
---|---|---|
committer | Angelo Rossi <angelo.rossi.homelab@gmail.com> | 2023-06-21 12:04:16 +0000 |
commit | b18347ffc9db9641e215995edea1c04c363b2bdf (patch) | |
tree | f3908dc911399f1a21e17d950355ee56dc0919ee /benchmarks/dc27.dat |
Initial commit.
Diffstat (limited to 'benchmarks/dc27.dat')
-rw-r--r-- | benchmarks/dc27.dat | 524 |
1 files changed, 524 insertions, 0 deletions
diff --git a/benchmarks/dc27.dat b/benchmarks/dc27.dat new file mode 100644 index 0000000..9ea0614 --- /dev/null +++ b/benchmarks/dc27.dat @@ -0,0 +1,524 @@ +BEGIN NEW DATA CASE
+C BENCHMARK DC-27
+C Test of "CABLE CONSTANTS", 1st for an underground cable, then for an
+C overhead line. For the cable, two of the phases have both cores and
+C sheaths, whereas the 3rd has only the core. A homogeneous earth model is
+C assumed. Both modal and phase-domain output is illustrated.
+C DIAGNOSTIC 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 9
+C 2 August 2002, add plot of cable cross-section on the screen:
+C $DEPOSIT, KROSEC=1, { Use SPY DEPOSIT to change this variable of STARTUP
+CABLE CONSTANTS
+ 2 -1 3 0 1 1 1
+ 2 2 1
+ 25.4E-3 45.6E-3 50.8E-3 55.9E-3
+ 6.8912E-8 1. 1. 3.52 6.8662E-7 1. 1. 3.3
+ 25.4E-3 45.6E-3 50.8E-3 55.9E-3
+ 6.8912E-8 1. 1. 3.52 6.8662E-7 1. 1. 3.3
+ 25.4E-3 45.6E-3
+ 6.8912E-8 1. 1. 3.52
+ 0.75 0.0 0.75 0.3 0.75 0.15
+ 20.0 1000.0
+C Impedance matrix [ Z ] in [ohm/m] follows :
+C 1.0871342E-03 9.7123603E-04 9.7126618E-04 9.7295525E-04 9.7123603E-04
+C 1.0433822E-02 7.2285319E-03 8.0995634E-03 9.5255505E-03 7.2285319E-03
+C Admittance matrix [ Y ] in [mho/m] follows :
+C 0.0000000E+00 0.0000000E+00 0.0000000E+00 0.0000000E+00 0.0000000E+00
+C 2.1027008E-06 0.0000000E+00 0.0000000E+00 -2.1027006E-06 0.0000000E+00
+C Transpose of the current transformation matrix [Ti] follows. This is the inve
+C 0.0019301 0.0019301 0.0795508 0.4608603 0.4608604
+C 94.5057220 94.5057220 1.0795423 -0.4399059 -0.4399060
+C Voltage transformation matrix [Tv]. This gives the mapping from modal to phas
+C 0.9983159 0.9985634 0.1872344 1.0000001 0.9999997
+C 1.3742625 11.7389965 -128.8459167 -0.0000002 0.0000385
+C Characteristic impedance matrix [Zc] in phase variables, in [ohm]:
+C 46.5745659 11.1852903 15.2132778 24.9359932 11.2755394
+C -4.8109016 -1.6719475 -2.0647478 -0.4119074 -1.1299886
+C Modal Propagation Modal impedance Modal
+C Mode attenuation velocity real imaginary susceptance
+C [ db/km ] [ m/sec ] [ ohms / meter ] [mho/meter]
+C 1 2.81088E-01 1.34059E+07 1.188315E-03 8.349145E-03 2.617198E-05
+C 2 1.38270E-01 3.78950E+07 2.186609E-04 1.137942E-03 2.394342E-05
+C 3 3.73454E-02 8.94327E+07 3.196348E-04 2.227090E-03 2.201588E-06
+C 4 1.05997E-01 1.34007E+08 3.100181E-04 4.750426E-04 4.128194E-06
+C 5 1.10538E-01 1.35064E+08 3.239154E-04 4.686100E-04 4.072995E-06
+BLANK card ending frequency cards
+C $DEPOSIT, KROSEC=0, { Use SPY DEPOSIT to cancel the change at start of subcase
+C Begin 2nd subcase, for overhead line. This is untransposed, with one
+C conductor per phase. This is a single 3-phase circuit with two ground
+C wires. The 3-layer ("Nakagawa") stratified earth model is assumed.
+ 1 0 1 99 1
+ 3 2 4 1
+ 8.74E-3 1.974E-3 6.18E-3 0. 0.4 6.78E-3
+ 3.78E-8 1. 5.36E-8 1.
+ 25. 12.5 0. 25. 12.5 14.
+ 25. 12.5 28. 35. 17.5 3.
+ 35. 17.5 25.
+ 200. 1.E+05 80000.
+ .5 2.5 200. 1000.
+ 1.0 1.0 1.0 10.0 10.0 10.0
+C Resistance [ R ] in [ohm/m] and inductance [ L ] in [henry/m] follows :
+C 3.6631241E-02 3.3899128E-02 3.0530494E-02
+C 1.0974409E-06 2.2856192E-07 1.1843866E-07
+C Conductance [ G ] in [mho/m] and capacitance [ C ] in [farad/m] follows :
+C 0.0000000E+00 0.0000000E+00 0.0000000E+00
+C 1.1469370E-11 -1.4910953E-12 -3.6612786E-13
+C Transpose of the current transformation matrix [Ti] follows. This is the inve
+C 0.3508662 0.3422453 0.3508658
+C 0.2195983 2.4146881 0.2195537
+C Voltage transformation matrix [Tv]. This gives the mapping from modal to phas
+C 0.9379887 0.9999999 0.4877141
+C -1.4748241 0.0000000 -177.8047791
+C Characteristic impedance matrix [Zc] in phase variables, in [ohm]:
+C 312.2572632 53.8941574 24.6474152
+C -7.9390864 -7.2640944 -6.5128512
+C Modal Propagation Modal impedance Modal
+C Mode attenuation velocity real imaginary susceptance
+C [ db/km ] [ m/sec ] [ ohms / meter ] [mho/meter]
+C 1 1.10051E+00 2.69766E+08 2.544782E-02 3.395038E-01 1.597196E-05
+C 2 9.21221E-02 2.93771E+08 3.050453E-03 3.075625E-01 1.487293E-05
+C 3 1.39649E-02 2.99027E+08 9.903153E-03 3.568964E-01 1.236180E-05
+BLANK card ending frequency cards
+BLANK card ending "CABLE CONSTANTS" data subcases
+BEGIN NEW DATA CASE
+C August, 1994. Prof. Akihiro Ametani has left after 3 weeks of work
+C at BPA to install his new CABLE PARAMETERS program. There are 18
+C standard test cases for this, and these will be split between the
+C ends of DC-27 and DC-28. Begin with the 6 examples for overhead
+C lines: 11A, 11G0, 11G1, 11G3, 11Y2, and 11A' (with prime meaning
+C modification). Then will come 4 pipe-type cable examples.
+C 1st of 6 overhead line examples: CASE11A.DAT
+CABLE CONSTANTS
+CABLE PARAMETERS
+C KOLW27 KOLS27 E also?
+MATRIX PRECISION 10 1 { Optimally encode old F-field
+C 4 December 2003, optional local KOLWID and KOLSEP of optimal encoding
+C are read from columns 25-40. Variables are local to overlay 27, and are
+C carried in LABL27. The default values (for default use, see DC-28) are
+C KOLW27 = 10 and KOLS27 = 2 (column width of 10 including 2 blanks to
+C separate matrix columns). Here, using KOLS27 = 1 gives one more digit
+C of precision at the expense of blank column separation. Since matrices
+C are visually more appealing with 2 blank separator bytes, the default
+C values will be reset on the following subcase.
+C Ze
+C MATRIX OUTPUTS 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
+C 22 December 2003, optional preceding definition of KZFL27(16) is added.
+C This integer vector controls which matrices are to be outputed (to either
+C LUNIT6 or separate disk files, or both), and what coordinates are to be
+C used (e.g., a COMPLEX matrix, a matrix of real parts, a matrix of
+C imaginary parts, a matrix of magnitudes, or a matrix of angles).
+C Index Cols. Symbol Labeling of matrix in the LUNIT6 file
+C ----------------------------------------------------------------------
+C 1 17-20 P Complex potential coefficient
+C 2 21-24 Pt Transposed potential coefficient
+C 3 25-28 Ze Earth impedance ZE, in ohm/m
+C 4 29-32 Zc Conductor internal impedance ZC, in ohm/m
+C 5 33-36 Zs Space impedance ZS, in ohm/m
+C 6 37-40 Presently unused (reserved for later use)
+C 7 41-44 Zt Total impedance [Zc], in ohm/m
+C 8 45-48 Yt Total admittance [Yc], in mho/m
+C 9 49-52 Zph Characteristic impedance matrix [Zc] in phase variables, in [ohm]
+C 10 53-56 Ti The current transformation matrix [Ti] follows. ...
+C 11 57-60 Tv Voltage transformation matrix [Tv]. ...
+C ----------------------------------------------------------------------
+C 12 61-64 Comp Complex matrix, with each cell a complex pair
+C 13 65-68 Real Only the real part of the complex matrix
+C 14 69-72 Imag Only the imaginary part of the complex matrix
+C 15 73-76 Mag Only the magnitudes of the complex elements
+C 16 77-80 Angle Only the angles in degrees of the complex elements
+ 1 0 2 0 1 1 0 0 0 1 0 0
+ 3 0 1 0
+79.9916E-631.7050E-3
+23.7025E-5 1.0
+ 1 0 1 0
+19.6350E-615.7080E-3
+90.5019E-5 1.0
+ 11.35 11.35 -0.65 11.35 11.35 0.00
+ 11.35 11.35 0.65 12.35 12.35 0.00
+ 50. 4.0E06
+C Total impedance [Zc]
+C 3.81674E-01 3.64103E-01 3.63346E-01 3.49908E-01
+C 4.26910E+01 1.82546E+01 1.47757E+01 1.54036E+01
+C
+C Total admittance [Yc]
+C 0.00000E+00 0.00000E+00 0.00000E+00 0.00000E+00
+C 2.18090E-04 -6.35291E-05 -3.38427E-05 -3.80217E-05
+C
+C Characteristic impedance matrix [Zc] in phase variables, in [ohm]:
+C 506.78659 215.40545 173.91332 181.49599
+C -2.25771 -2.15298 -2.14844 -2.06889
+C
+C Modal transformation matrices follow. These are complex, with the real part displayed above the imaginary part.
+C Transpose of the current transformation matrix [Ti] follows. This is the inverse of the voltage transformation matrix.
+C By definition, [Ti] gives the mapping from modal to phase variables: i-phase = [Ti] * i-mode
+C 0.27659 -0.26181 -0.34850 -0.50000
+C 0.00030 0.00062 -0.00015 0.00000
+C
+C Voltage transformation matrix [Tv]. This gives the mapping from modal to phase variables: v-phase = [Tv] * v-mode
+C 1.00000 -0.29619 -0.41855 -1.00000
+C 0.00038 0.00155 -0.00035 0.00000
+C
+C MODE ATTENUATION VELOCITY IMPEDANCE (OHM/M) ADMITTANCE (S/M)
+C NO. (DB/KM) (M/MIC.S) REAL IMAG. REAL IMAG.
+C 1 5.74605E+00 297.25 3.68397E-01 2.35412E+01 0.00000E+00 3.03655E-04
+C 2 3.60799E-01 299.64 2.43100E-02 2.45439E+01 0.00000E+00 2.86632E-04
+C 3 2.70957E-01 299.68 1.29042E-02 1.73460E+01 0.00000E+00 4.05472E-04
+C 4 2.39123E-01 299.69 9.16390E-03 1.39576E+01 0.00000E+00 5.03865E-04
+BLANK card ending frequency cards within CABLE PARAMETERS
+C 27 December 2003, changes to MAIN27 made it possible to stack subcases
+C within CABLE PARAMETERS. To demonstrate this, the following exit and
+C re-entry (4 non-comment data cards) will be commented out. The answer
+C is unchanged. Although not recommended, such stacking does now work.
+C BLANK card ending CABLE CONSTANTS data subcases
+C BEGIN NEW DATA CASE
+C CABLE CONSTANTS
+C CABLE PARAMETERS
+C KOLW27 KOLS27 E also?
+MATRIX PRECISION 10 2 { Optimally encode old F-field
+C 4 December 2003, optional local KOLWID and KOLSEP of optimal encoding
+C are read from columns 25-40. Values 10 and 2 above serve to restore the
+C default values. These replace values 10 and 1 of the preceding subcase.
+ 1 0 2 0 1 0 0 0 0 0 0 0
+ 3 0 1 0
+ 5.046E-3 0.0
+ 1.896E-8 1.0
+ 1 0 1 0
+ 2.50E-3 0.0
+ 1.777E-8 1.0
+ 11.35 11.35 -0.65 11.35 11.35 0.00
+ 11.35 11.35 0.65 12.35 12.35 0.00
+ 50. 4.0E06
+C MODE ATTENUATION VELOCITY IMPEDANCE (OHM/M) ADMITTANCE (S/M)
+C NO. (DB/KM) (M/MIC.S) REAL IMAG. REAL IMAG.
+C 1 5.74605E+00 297.25 3.68397E-01 2.35412E+01 0.00000E+00 3.03655E-04
+C 2 3.60799E-01 299.64 2.43100E-02 2.45439E+01 0.00000E+00 2.86632E-04
+C 3 2.70957E-01 299.68 1.29042E-02 1.73460E+01 0.00000E+00 4.05472E-04
+C 4 2.39123E-01 299.69 9.16391E-03 1.39576E+01 0.00000E+00 5.03865E-04
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 3rd of 6 overhead line examples: CASE11G1.DAT
+CABLE CONSTANTS
+CABLE PARAMETERS
+ 1 0 2 0 1 0 0 0 1 0 0 0
+ 3 0 1 0
+ 5.046E-3 0.0
+ 1.896E-8 1.0
+ 1 0 1 0
+ 2.50E-3 0.0
+ 1.777E-8 1.0
+ 11.35 11.35 -0.65 11.35 11.35 0.00
+ 11.35 11.35 0.65 12.35 12.35 0.00
+ 50. 4.0E06
+C MODE ATTENUATION VELOCITY IMPEDANCE (OHM/M) ADMITTANCE (S/M)
+C NO. (DB/KM) (M/MIC.S) REAL IMAG. REAL IMAG.
+C 1 3.17679E+00 298.37 1.79566E-01 2.06778E+01 0.00000E+00 3.43133E-04
+C 2 2.70975E-01 299.68 1.30187E-02 1.74987E+01 0.00000E+00 4.01933E-04
+C 3 2.39123E-01 299.69 9.16391E-03 1.39576E+01 0.00000E+00 5.03865E-04
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 4th of 6 overhead line examples: CASE11G3.DAT
+CABLE CONSTANTS
+CABLE PARAMETERS
+ 1 0 2 0 1 0 0 0 3 0 0 0
+ 3 0 1 0
+ 5.046E-3 0.0
+ 1.896E-8 1.0
+ 1 0 1 0
+ 2.50E-3 0.0
+ 1.777E-8 1.0
+ 11.35 11.35 -0.65 11.35 11.35 0.00
+ 11.35 11.35 0.65 12.35 12.35 0.00
+ 50. 4.0E06
+C MODE ATTENUATION VELOCITY IMPEDANCE (OHM/M) ADMITTANCE (S/M) CHARACT. IMP. (OHM) CHARACT. ADMIT. (S)
+C NO. (DB/KM) (M/MIC.S) REAL IMAG. REAL IMAG. REAL IMAG. REAL IMAG.
+C 1 8.29798E-01 299.42 7.35361E-02 3.23051E+01 0.00000E+00 2.18090E-04 384.874 -0.438 2.59825E-03 2.95720E-06
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 5th of 6 overhead line examples: CASE11Y2.DAT
+CABLE CONSTANTS
+CABLE PARAMETERS
+ 1 0 2 0 1 0 0 0 0 0 2 0
+ 3 0 1 0
+ 5.046E-3 0.0
+ 1.896E-8 1.0
+ 1.E-15 0.0 1.E-15 0.0 1.E-15 0.0
+ 1 0 1 0
+ 2.50E-3 0.0
+ 1.777E-8 1.0
+ 8.333E-4 0.0
+ 11.35 11.35 -0.65 11.35 11.35 0.00
+ 11.35 11.35 0.65 12.35 12.35 0.00
+ 50. 4.0E06
+C MODE ATTENUATION VELOCITY IMPEDANCE (OHM/M) ADMITTANCE (S/M)
+C NO. (DB/KM) (M/MIC.S) REAL IMAG. REAL IMAG.
+C 1 1.11101E+03 165.22 3.71110E-01 4.66305E+01 8.33317E-04 1.52015E-04
+C 2 3.17749E+00 298.37 1.79366E-01 2.06500E+01 0.00000E+00 3.43588E-04
+C 3 2.70975E-01 299.68 1.30187E-02 1.74987E+01 0.00000E+00 4.01933E-04
+C 4 2.39123E-01 299.69 9.16391E-03 1.39576E+01 0.00000E+00 5.03865E-04
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 6th of 6 overhead line examples: CASE11A'.DAT
+CABLE CONSTANTS
+CABLE PARAMETERS
+ 1 0 1 0 1 0 0 0 0 1 0 0
+ 3 1 1 1
+79.9916E-631.7050E-30.0000E+0019.6350E-615.7080E-3 0.0
+23.7025E-5 1.090.5019E-5 1.
+ 11.35 11.35 -0.65 11.35 11.35 0.00
+ 11.35 11.35 0.65 12.35 12.35 0.00
+ 50. 4.0E06
+C MODE ATTENUATION VELOCITY IMPEDANCE (OHM/M) ADMITTANCE (S/M)
+C NO. (DB/KM) (M/MIC.S) REAL IMAG. REAL IMAG.
+C 1 3.17679E+00 298.37 1.79566E-01 2.06778E+01 0.00000E+00 3.43134E-04
+C 2 2.70975E-01 299.68 1.30186E-02 1.74987E+01 0.00000E+00 4.01933E-04
+C 3 2.39123E-01 299.69 9.16390E-03 1.39576E+01 0.00000E+00 5.03865E-04
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 1st of 4 pipe-type cable examples: CASE3G0.DAT
+C Results of this case changed on March 2, 2001 after implementing the
+C correction that Prof. Ametani made on February 17, 2001.
+C This correction only affects cables having 3 layers of conductors: core,
+C sheath and armor.
+CABLE CONSTANTS
+CABLE PARAMETERS
+C Beginning 28 September 2002, users are allowed to monitor convergence of
+C Prof. Ametani's eigenvalue calculation. For high order, this will be seen
+C automatically. This is important because computation may be slow. But how
+C large is large? MONMIN is the variable, and the user has control via a
+C new optional declaration that must (if present) precede miscellaneous data.
+C In the following, MAXITR = maximum number of iterations for an eigenvalue;
+C MONMIN = minimum order for the new eigenvalue printout;
+C ITROUT = frequency of printout within eigenval iteration;
+C EPSLNA = convergence tolerance for eigenvalue iteration.
+C This data subcase is of order 10, so is big enough for meaningful printout.
+C Default values are: 100 50 1 1.E-8
+C MAXITR MONMIN ITROUT EPSLNA
+EIGEN CONTROLS 85 5 1 1.E-8
+C 3 -1 3 0 0 0 0 1 0 0 0 0
+ 3 -1 3 0 1 0 0 1 0 0 0 0
+ 1.850 1.860 1.870 1.00E-7 1.0 1. 1.
+1.17183738-29.9354891.18391480-38.1912031.32171262-33.629952
+ 3 3 3
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 20.0 0.0
+ 33. 500.0E03
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 2nd of 4 pipe-type cable examples: CASE3G1.DAT
+C Results of this case changed on March 2, 2001 after implementing the
+C correction that Prof. Ametani made on February 17, 2001.
+C This correction only affects cables having 3 layers of conductors: core,
+C sheath and armor.
+CABLE CONSTANTS
+CABLE PARAMETERS
+C MAXITR MONMIN ITROUT EPSLNA
+EIGEN CONTROLS -85 -5 -1 -1.E-8
+C Default values are: 100 50 1 1.E-8
+C 17 January 2004, the preceding is added to illustrate rejection of any bad
+C value. Here, a minus sign has been added to each parameter. Each will be
+C rejected, and this means no change. So, MAXITR will remain at value 85,
+C MONMIN will remain at value 5 (compare with default values of 100 and 50,
+C respectively).
+C 3 -1 3 0 0 0 0 1 1 0 0 0
+ 3 -1 3 0 1 0 0 1 1 0 0 0
+ 1.850 1.860 1.870 1.00E-7 1.0 1. 1.
+1.17183738-29.9354891.18391480-38.1912031.32171262-33.629952
+ 3 3 3
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 20.0 0.0
+ 33. 500.0E03
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 3rd of 4 pipe-type cable examples: CASE3G4.DAT
+CABLE CONSTANTS
+CABLE PARAMETERS
+C KOLW27 KOLS27 E also?
+MATRIX PRECISION 10 2 BOTH { Optimally encode both E & F
+C About preceding 2 lines, which were added 6 December 2003: KOLW27 and KOLS27
+C are unchanged. But added BOTH in 45-48 is the request to have the real part
+C optimally encoded rather than ordinary E-field encoded. I.e., treat the real
+C part the same as the imaginary part of the matrix for printed output.
+C 3 -1 3 0 0 0 0 1 4 0 0 0
+ 3 -1 3 0 1 1 0 1 4 0 0 0
+ 1.850 1.860 1.870 1.00E-7 1.0 1. 1.
+1.17183738-29.9354891.18391480-38.1912031.32171262-33.629952
+ 3 3 3
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 20.0 0.0
+ 33. 500.0E03
+C Characteristic impedance matrix [Zc] in phase variables, in [ohm]:
+C 33.72483 0.00000 0.00000 4.62992 0.00000 0.00000
+C -0.11456 -0.00001 -0.00001 -0.06850 -0.00001 -0.00001
+C
+C MODE ATTENUATION VELOCITY IMPEDANCE (OHM/M) ADMITTANCE (S/M)
+C NO. (DB/KM) (M/MIC.S) REAL IMAG. REAL IMAG.
+C 1 2.18897E-01 197.36 1.46645E-03 4.63124E-01 0.00000E+00 5.47097E-04
+C 2 2.18897E-01 197.36 1.46645E-03 4.63124E-01 0.00000E+00 5.47097E-04
+C 3 2.18897E-01 197.36 1.46645E-03 4.63124E-01 0.00000E+00 5.47097E-04
+C 4 1.36719E+00 295.29 1.45751E-03 4.92463E-02 0.00000E+00 2.29785E-03
+C 5 1.36719E+00 295.29 1.45751E-03 4.92463E-02 0.00000E+00 2.29785E-03
+C 6 1.36719E+00 295.29 1.45751E-03 4.92463E-02 0.00000E+00 2.29785E-03
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 4th of 4 pipe-type cable examples: CASE3NP0.DAT
+C Results of this case changed on March 2, 2001 after implementing the
+C correction that Prof. Ametani made on February 17, 2001.
+C This correction only affects cables having 3 layers of conductors: core,
+C sheath and armor.
+CABLE CONSTANTS
+CABLE PARAMETERS
+C KOLW27 KOLS27 E also?
+MATRIX PRECISION 8 1 BOTH { Optimally encode both E & F
+C About preceding 2 lines, which were added 8 December 2003. This is the same
+C as the preceding subcase, but with the width minimized as an illustration.
+C There is no need; this is just an illustration.
+C 3 0 3 0 0 0 0 0 0 0 0 0
+ 3 0 3 0 1 0 0 0 0 0 0 0
+ 1.850 1.00E-7 1.0 1. 1.
+1.17183738-29.9354891.18391480-38.1912031.32171262-33.629952
+ 3 3 3
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 11.0E-3 30.60E-3 63.80E-3 65.80E-3 71.00E-3 71.80E-3 76.80E-3
+ 1.8365E-8 1.0 1.0 2.3 1.8365E-8 1.0 1.0 1.
+ 10.00E-8 1.0 1.0 8.0
+ 33. 500.0E03
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C Use preceding data of the 1st of 6 overhead line examples ( CASE11A.DAT )
+C to illustrate fitting associated with new frequency-dependence of Taku Noda
+C 1st of 2 NODA SETUP examples that are being added 6 October 1994
+C NODA SETUP, 1, { Request Taku Noda's ARMA model fitter. 1 ==> F-scan printout
+NODA SETUP { Request Taku Noda's ARMA model fitter. No printout of F-scan
+ { Output file name (blank requests use of default TAKUNODA.CCC)
+2nd of 2 such lines (any number are allowed).
+NODA SETUP END { Bound of fitter data; begin CABLE PARAMETERS data
+CABLE CONSTANTS
+CABLE PARAMETERS
+C KOLW27 KOLS27 E also?
+MATRIX PRECISION 10 2 BOTH { Optimally encode both E & F
+C The preceding 2 lines were added 8 December 2003. They cancel the narrow
+C columns of the preceding subcase. This is a return to default values.
+ 1 0 2 0 1 0 0 0 0 1 0 0
+ 3 0 1 0
+79.9916E-631.7050E-3
+23.7025E-5 1.0
+ 1 0 1 0
+19.6350E-615.7080E-3
+90.5019E-5 1.0
+ 11.35 11.35 -0.65 11.35 11.35 0.00
+ 11.35 11.35 0.65 12.35 12.35 0.00
+ 50. 10. 5 10 600.
+ 50. 1.E8 600.
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending CABLE CONSTANTS data subcases
+BEGIN NEW DATA CASE
+C 2nd of 2 NODA SETUP examples that are being added 6 October 1994
+C The preceding was for an overhead line. This is for a single-phase
+C cable (core and sheath). Cable data came from CESI (see DCNEW-6).
+NODA SETUP { Request Taku Noda's fitter, for which data follows
+ { Output file name (blank requests use of default TAKUNODA.CCC)
+2nd of 2
+NODA SETUP END { Bound of fitter data; begin CABLE PARAMETERS data
+CABLE CONSTANTS
+CABLE PARAMETERS { Transfer to new (August, 1994) cable constants code
+C MISCELLANEOUS DATA CARD
+ 2 -1 1 0 1 0 0 0
+C CARDS INDICATING NUMBER OF CONDUCTORS PER SC COAXIAL CABLE
+ 2
+C GEOMETRICAL AND PHYSICAL DATA CARDS
+ .0206 .02865 .06395 .0689 .0775
+ 1.775E-8 1. 1. 3.5 9.1E-8 1. 1. 2.25
+C CROSS-SECTION LOCATION CARD
+ 1.05 0.
+C EARTH RESISTIVITY AND FREQUENCY CARDS
+ 300. 10. 5 10 600.
+ 300. 1.E8 600.
+BLANK card ending frequency cards of imbedded "LINE PARAMETERS" data case
+BLANK card ending "CABLE PARAMETERS" data cases
+BLANK card ending "CABLE CONSTANTS" data cases
+BEGIN NEW DATA CASE
+C Final subcase is same as 1st subcase of CABLE PARAMETERS except that
+C it illustrates omission of preceding CABLE CONSTANTS and following
+C blank to terminate that otherwise-unused routine. See October, 1997,
+C newsletter story explaining this improvement. WSM, 13 August 1997
+CABLE PARAMETERS { Note there is no preceding CABLE CONSTANTS request
+ 1 0 2 0 1 0 0 0 0 1 0 0
+ 3 0 1 0
+79.9916E-631.7050E-3
+23.7025E-5 1.0
+ 1 0 1 0
+19.6350E-615.7080E-3
+90.5019E-5 1.0
+ 11.35 11.35 -0.65 11.35 11.35 0.00
+ 11.35 11.35 0.65 12.35 12.35 0.00
+ 50. 4.0E06
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending "CABLE PARAMETERS" data cases
+BEGIN NEW DATA CASE
+C This is an example of a system which is a combination of an
+C overhead line and an underground line.
+C In October, 1998, Prof. Aki Ametani provided this data case as an
+C illustration for the calculation of the mutual earth-return
+C impedance of a system which is a combination of overhead and
+C underground conductors (lines or cables). A paper, co-authored
+C by Prof. Ametani, S. Yamaguchi, and N. Nagaoka, titled "Mutual
+C Impedance between Overhead and Underground Cables" is to be
+C presented at the 1998 EEUG meeting on November 9-10
+C
+CABLE CONSTANTS
+CABLE PARAMETERS
+ 1 0 1 0 1 0 0 0 0 0 0 0
+C ITY ISYS NPC IEAR KMOD
+ 2 0 1 0
+C NP NG KBP KBG
+ .4300E-01 0.00 0.0 0.0 0.0 0.0
+C ROUTp RINp ROUTg RINg SEPp SEPg
+ .1690E-07 1.0
+C RHOp MUp RHOg MUg
+ 1.00 1.00 0.00 -0.1 -0.1 0.0
+C VTOWER1 VMID1 HORIZ1 VTOWER2 VMID2 HORIZ2
+ 100. 10.000 8 1
+C RHO FREQ IDEC IPNT
+BLANK card ending frequency cards within CABLE PARAMETERS
+BLANK card ending "CABLE PARAMETERS" data cases
+BLANK card ending "CABLE CONSTANTS" data cases
+BEGIN NEW DATA CASE
+BLANK
+
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