Relation of height of window to width of window is 2
to 4 Hw / Ww = 2 to 4 |
Area of yoke = ( 1.15 to 1.25 ) Agi for hot rolled
steel = Agi for cold rolled steel |
The diameter of circumscribing circle is directly proportional
to √ Ai Where Ai = Core Area |
The length of mean turns of conductors wound on cold
rolled steel is 0.817 times that of hot rolled steel Volume of conductor in cold rolled steel is 18.3%
lesser than that of hot rolled steel = ( 1 – 0.817 ) × 100 |
MMF of primary winding = NPIP MMF of secondary winding = NSIS
Voltage regulation of transformer = Er Cos Φ + Ex Sin Φ + ½ ( Er
Sin Φ – Ex Cos Φ )2 Where Er = Per unit resistance = IPRP
/ VP Ex = Per unit reactance = IPXP
/ VP |
The average value of flux density in the duct = Ba
/ 2 |
Short circuit fault current = I / Ex Where I = RMS fault current Ex = Per unit leakage reactance |
Ratio of maximum radial force under
worst fault condition to maximum radial force under normal condition Fr ( max ) f / Fr ( max )
n = 2 / Ex2 Where Fr ( max ) f = Radial force under fault
condition Fr ( max ) n = Radial force under normal
condition If one winding is only 5% shorter than other winding,
it produces large axial force. |
No load current I0 = √ ( Iw2 + Iµ2
) Where Iw = Loss component of no load current Iµ = Magnetizing current |
RMS value of magnetizing current Iµ = AT0 ( N0 I0
) / √ 2 NP Where AT0 = Total primary turns NP = Primary turns Magnetizing current Iµ = Magnetizing VA per kg × Weight of
core / Number of phases × Voltage per phase |
Eddy current loss We = kf2Bmax2 If the supply voltage is kept constant , ( f Bmax
) remain constant therefore the eddy current loss remains constant in spite
of frequency is changed |
Hysteresis loss Wh = k fBmax2 If the supply voltage is constant, product of f Bmax
remains constant Wh = k ( f Bmax ) Bmax Let f Bmax = k1 constant Bmax = k1 / f Wh = kk12 / f If the supply voltage is kept constant, hysteresis
loss decreases with increases in the frequency. |
The leakage reactance increases with increase in frequency.
The effective resistance increases with increases in frequency. |
The copper losses don’t depend on supply frequency. |
Effect of frequency on flux density if
the supply voltage is kept constant V2 = 4.44 f2Φmax2N2 V1 = 4.44f1Φmax1N1 Let us consider that frequency f1( 50 Hz )
changes to f2 ( 40 Hz ) Φmax2f2 = Φmax1f1 Φmax2 = ( f1 / f2 )
Φmax1 = ( 50 / 60 ) Φmax1 Φmax2 = ( 0.82 ) Φmax1 |
The eddy current losses do not affect with change in
frequency. |
Copper loss varies as the square of the
output WC2 / WC1 = ( output in 2nd
case )2 / ( output in 1st case )2 The power rating of transformer increases with
increase in frequency. |
Specific heat dissipation due to
convection of oil λconv = 40.3 ( θ / H )1.4 Where θ = Temperature difference of surface relative to oil H = Height of dissipating surface |
Effect of Wc / Wi
on overload capacity of transformer Case 1 : Wc / Wi = 1 Case 2 : Wc / Wi = 2 At 20% overlaod Case 1 Total loss at overload / Total load at full load [ ( 2 )2 × 1 ] + 1 / ( 1 + 1 ) = 2.5 Case 2 Total loss at overload / Total load at full load [ ( 2 )2 × 1 ] + 1 / ( 2 + 1 ) = 3 Therefore the overload losses in the two cases are
2.5 : 3 therefore the transformer with higher Wc / Wi
is less as compared to sustain overload |
Heating time constant Th = Gh / Sλ Where G = Weight h = Specific heat λ = Specific heat dissipation Th = Gh θ / Q ( ⸫ Sλ = Q / θ ) The heating time constant of oil is about 30 times
to that of winding. |
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