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IMPEDANCE
Siechem
Wires & Cables
Electrical impeda nce is the measu re of the opposition of an electric current to the
energy flow when voltage is applied. In quantitative terms, it is a complex ratio of the
voltage to the current in an alterna ting current (AC) circuit. Impedance extends the concept
of resista nce to AC circuits, and possesses both magnitude and phase, unlike resista nce
which has only magnitude
The phase impedance Z of a single core cables is given by
Z=.JR.2
+x2
(Q/km)
Where,
R= A.C. resistance at operating temperature (Q/km)
X= reacta nce (Q/km) (X = 2nfL x lQ-3)
f = frequency (Hz)
L= inductance (mH/km)
Balanced pair
For unshielded twisted pair
= 1016.ft
20
c
For shielded twisted pair
z 276 [l.2D]
0 .J& g fd
For overall shielded &cabled
z =347lo<>(I.SD]
0 .J& b fd
Where,
C = Mutual capacitance (pF/ft.)
d = Diameter of the conductor (in.)
D =Diameter over the insulation (in.)
E: =Insulation dielectric constant (seeTable 2)
f =Stranding factor (see Table 1)
Zo=Characteristic impedance
Table 1 Table 2
Siechem
Wires & Cables
Material Dielectric
Constant
t: fnF/ft)
Velocity of
Propagation
Yr (%)
ECTFE (Halar) 2.60 63
PFA (Teflon) 2.15 68
PVC 5.00 45
PVC (Semi-rie:id) 3.60 53
PVDF (Kynar,
SOLEF)
7.70 36
Polvethvlene 2.29 66
Polvoroovlene 2.25 67
Polvurethane 6.50 39
Rubber - butvl 4.0 50
Rubber - natural 5.0 45
Rubber - SBR 4.0 50
Rubber -silicone 3.1 57
TFE Teflon 2.1 69
TPE 5.0 45
Teflon 2.1
0 69
Tefzel 2.6 62
No.of
Strands
Stranding Factor
f
1 1
.000
7 0.939
1
9 0.970
37 0.980
61 0.985
91 0.988

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Impedance calculation by Rohit Damodaran

  • 1. = 1 0 IMPEDANCE Siechem Wires & Cables Electrical impeda nce is the measu re of the opposition of an electric current to the energy flow when voltage is applied. In quantitative terms, it is a complex ratio of the voltage to the current in an alterna ting current (AC) circuit. Impedance extends the concept of resista nce to AC circuits, and possesses both magnitude and phase, unlike resista nce which has only magnitude The phase impedance Z of a single core cables is given by Z=.JR.2 +x2 (Q/km) Where, R= A.C. resistance at operating temperature (Q/km) X= reacta nce (Q/km) (X = 2nfL x lQ-3) f = frequency (Hz) L= inductance (mH/km) Balanced pair For unshielded twisted pair = 1016.ft 20 c For shielded twisted pair z 276 [l.2D] 0 .J& g fd For overall shielded &cabled z =347lo<>(I.SD] 0 .J& b fd Where, C = Mutual capacitance (pF/ft.) d = Diameter of the conductor (in.) D =Diameter over the insulation (in.) E: =Insulation dielectric constant (seeTable 2) f =Stranding factor (see Table 1) Zo=Characteristic impedance
  • 2. Table 1 Table 2 Siechem Wires & Cables Material Dielectric Constant t: fnF/ft) Velocity of Propagation Yr (%) ECTFE (Halar) 2.60 63 PFA (Teflon) 2.15 68 PVC 5.00 45 PVC (Semi-rie:id) 3.60 53 PVDF (Kynar, SOLEF) 7.70 36 Polvethvlene 2.29 66 Polvoroovlene 2.25 67 Polvurethane 6.50 39 Rubber - butvl 4.0 50 Rubber - natural 5.0 45 Rubber - SBR 4.0 50 Rubber -silicone 3.1 57 TFE Teflon 2.1 69 TPE 5.0 45 Teflon 2.1 0 69 Tefzel 2.6 62 No.of Strands Stranding Factor f 1 1 .000 7 0.939 1 9 0.970 37 0.980 61 0.985 91 0.988