Abstract
Power inductors are used for compensating VAR generated by long EHV transmission lines and in electronic circuits. For the EHV-lines, the rating of the inductor is decided upon by techno-economic considerations on the basis of the line-susceptance. It is a high voltage high current device, absorbing little active power and large reactive power. The cost is quite high- hence the design should be made cost-optimally. The 3-phase power inductor is similar in construction to a 3-phase core-type transformer with the exception that it has only one winding per phase and each limb is provided with an air-gap, the length of which is decided upon by the inductance required. In this paper, a design methodology based on sequential gradient search technique and the corresponding algorithm leading to cost-optimal design of a 3-phase EHV power inductor has been presented. The case-study has been made on a 220 kV long line of NHPC running from Chukha HPS to Birpara of Coochbihar.
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Appendices
Appendix 1
[Subroutine for the Design of Power Inductor]
Input \( S \leftarrow MVAR \) to be compensated \( S^{'} \leftarrow 1000 \times S/2 \) | // rating of the inductor in KVA |
Input \( f,V,K,R_{w} ,K_{s} \) | // frequency, line voltage, emf constant, |
// window height/width ratio, stacking factor | |
Input \( K_{w} ,K_{c} ,B_{m} ,\delta \) | // window space factor, constant depending on no of steps, |
// maximum flux density, current density (A/mm2) | |
\( E_{t} \leftarrow K\sqrt {S^{'} } \) | // emf per turn, V |
\( V_{p} \leftarrow V/\sqrt 3;\,\,N \leftarrow V_{p} /E_{t} \) | // phase voltage, no of turns |
\( \phi_{m} \leftarrow E_{t} /(4.44f) \); \( I = s \times 10^{6} /(3V_{p} ) \) | // maximum value of flux, current |
\( A_{i} \leftarrow \phi_{m} /B_{m};\,\,\,A_{gi} \leftarrow A_{i} /K_{s} \,\,;\,\,a_{c} \leftarrow I/\delta \) | // net/gross area of iron, conductor area |
Input \( N_{st} ,K_{1} \ldots \) | // number of core steps, corresponding length coefficients |
\( d \leftarrow \sqrt {A_{gi} /K_{c} };\,\,a \leftarrow K_{1} d \) | // diameter of the fictitious circle round the core; |
// length of the largest core step | |
\( A_{w} \leftarrow S^{{\prime }} /3.33fB_{m} A_{i} K_{w} \delta \times 10^{3} \) | // window area |
\( W_{w} \leftarrow \sqrt {A_{w} /R_{w} };\,\,H_{w} \leftarrow R_{w} W_{w} \) | // window width, height |
\( D_{c} \leftarrow W_{w} + d;\,\,W = 2D_{c} + a \) | // distance between core centres, total length of the core |
\( A_{gy} \leftarrow A_{gi} ;\,\,\,W_{y} \leftarrow a\,\,\,\,\,\,\, \) | // gross area, width of yoke |
\( \,H_{y} \leftarrow A_{gy} /W_{y} \) \( H \leftarrow H_{w} + 2H_{y} \) | // height of yoke, total height of core |
Input \( c_{w} ,c_{l} ,c_{h} \) | // tank clearances |
\( t_{w} \leftarrow D_{c} + 2c_{w} ;\,\,t_{l} \leftarrow W + 2c_{l} \,\,;\,\,t_{h} = H + c_{h} \) | // tank dimensions |
\( t_{a} \leftarrow 2(t_{l} + t_{w} )t_{h} + t_{l} t_{w} \) | // tank area for radiation |
Input \( p_{i} ,\rho ,\rho_{i} ,\rho_{c} \) | // specific iron loss, resistivity of conductor, density of iron, conductor |
\( V_{i} = (2W + 3H_{w} )A_{i} ;\,\,W_{i} = V_{i} \rho_{i} \,\,;\,\,\,P_{i} = W_{i} p_{i} \) | // volume, weight of iron, total iron loss |
\( L_{mt} = \pi (D_{c} - c_{wd} )\,\,;\,\,R \leftarrow \rho L_{mt} N/a_{c} \,\,;\,\,P_{c} = 3I^{2} R \) | // length of mean turn, resistance, total ohmic loss |
\( P_{ls} = P_{c} + P_{i} ;\,\,V_{c} = NL_{mt} a_{c} \times 10^{ - 6} \) | // total loss, volume of conductor |
Input \( V_{a} ,\lambda_{r} ,\lambda_{c} ,d_{t} \) | // velocity of air blast, dissipation by radiation, convection, |
// depth of tank wall | |
\( \lambda_{c}^{'} \leftarrow \lambda_{c} (1 + 1.3\sqrt {V_{a} } );\,\,V_{oil} = t_{h} t_{l} t_{w} K \) | // dissipation coefficient with air-blast, volume of oil |
// increased convection due to air-blast at 40 °C | |
\( x = t_{a} \lambda_{r} \times 40;\,\,t_{t} = (p_{ls} - x)/(\lambda_{c}^{'} \times 40) \) | // dissipation through radiation, total area of cooling tubes in the radiator |
\( Input\,s_{i} ,s_{c} ,s_{t} ,s_{o} \,\, - specific\,\,costs \) | |
\( C_{c} = V_{c} \rho_{c} s_{c} \); \( C_{i} = V_{i} \rho_{i} s_{i} \) | // cost of copper and iron |
\( C_{\tan k} \leftarrow (t_{a} + t_{t} )d_{t} \rho_{i} s_{t} \) | // cost of tank |
\( C_{oil} = V_{oil} s_{o} /1000 \) | // cost of transformer oil |
\( C_{t} = (C_{c} + C_{i} + C_{\tan k} + C_{oil} )(1 + OH) \) | // total cost along with overheads |
Appendix 2
[Cost Optimal design of a 3-Phase Power Inductor by Exhaustive Search]
Minimum cost 2,714,322/- is obtained for K = 0.43; Rw = 3.72
The design details of the cost-optimal power inductor:
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KVA-rating of the inductor = 15,000; rated line voltage = 220,000 V
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Nominal frequency = 50 Hz; connection: Y
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Conductor material: COPPER; current density = 3.2 A/sq. mm
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Core material CRGOS: flux-density = 1.7 Tesla
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Number of turns of the coil = 2933
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Current in coil = phase current = 39.368 A
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Current density = 3.2 A/sq. mm; cross section of the conductor = 12.302 sq. mm
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Net area of core iron = 0.1147357 sq. m; stacking factor = 0.972
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Gross area of core iron = 0.1180409 sq. m; 3-stepped core has been used.
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Diameter of the core circle = 0.4229 m
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Length of the core sides in m: = 0.383/0.299/0.179
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Area of the window = 0.3608 sq. m
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Window height/width ratio = 3.72; window height/width in m: 1.1709/0.3081
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Distance between core centres = 0.6909 m
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Width/height of yoke in m: 0.3827/0.3084
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Total length of core = 1.8448 m; total height of core = 1.7878 m
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Length of air-gap = 0.313 mm
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Volume of iron = 0.8264 cu. m; weight of iron = 6321.74 kg
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Iron loss/kg at this flux-density = 2.0966 W; iron loss = 13,254 W; % iron loss = 8.836E−02
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Mean length of turn = 1.7158 m; resistance of the coil = 9.0001 Ω
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Copper loss = 41,839.4 W; % copper loss = 0.27893; total % loss = 0.36729
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The tank length × width × height: 2.273 × 0.851 × 2.188
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Artificial cooling by air-blast on radiators is being used.
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The velocity of blast = 5 m/s; the blast constant (with some non-uniformity in blast) = 1.1
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The dissipation constant in = 35.234 W/sq. m/°C
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The number of elliptical tubes (75 × 25 mm) in the radiator = 110
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The cost of sheet metal/kg = Rs. 50/-
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The weight/cost of tank: 913.4537 kg; Rs. 45,673/-
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The cost of oil/litre = Rs. 40/-
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The volume/cost of oil: 4.231074 cu. m; Rs. 169,243/-
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Volume of iron = 0.82637 cu. m; weight of iron = 6321.7 kg
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Cost of iron/kg = Rs. 150/-; cost of iron = Rs. 948,261/-
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Volume of copper = 0.1857 cu. m; weight of copper = 1652.9 kg
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Cost of copper/kg = Rs. 450/-; cost of copper = Rs. 743,816/-
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Direct cost allowing 15% labour charge = Rs. 2,193,042/-
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Selling cost allowing 25% overhead = Rs. 2,741,302/-
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Basak, R., Das, A. & Sanyal, A. Cost Optimal Design of a Power Inductor by Sequential Gradient Search. J. Inst. Eng. India Ser. B 99, 413–418 (2018). https://doi.org/10.1007/s40031-018-0329-5
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DOI: https://doi.org/10.1007/s40031-018-0329-5