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Design: 125 kVA single phase transformer

Short answer

Core diameter 223.5 mm, limb 190.0×118.5 mm; window 137.5×300.6 mm (adjusted for coil clearance); yoke depth 190.0 mm, height 196.3 mm. Overall frame 693.3×551.0×190.0 mm. Leakage reactance calculation is not fully provided.

Design a 125 kVA, 50 Hz, 6600/400 V, 1-phase, core type oil immersed natural cooled distribution transformer. Given that: Maximum flux density in the core = 1.35 Wb/m²; Current density = 2.75 A/mm²; Core type = cruciform two stepped; Window space factor = 0.30; Stacking factor = 0.9; Ratio of window height to width 2.5; Take hot rolled steel sheet and area of yoke is 20% greater than area of core; Axial depth of L.V. winding = 268 mm; Axial depth of H.V. winding = 276 mm; Inside diameter of LV winding = 255 mm; Radial depth of LV winding = 14 mm; Radial depth of HV winding = 18 mm; Width of insulation between LV and HV = 11 mm; Outside diameter of LV winding = 293 mm; Inside diameter of HV winding = 314 mm; Outside diameter of HV winding = 351 mm. Calculate: i) Dimension of the core, window and yoke ii) Overall dimension of the frame iii) Leakage reactance of the transformer. Appropriate values for additional data required may be assumed if necessary.

Standard method (A.K. Sawhney, A Course in Electrical Machine Design): Et=KQE_t = K\sqrt{Q}, net core area ratio for the core type, output equation for the window, yoke depth = width of largest stamping. In a single-phase core type transformer half of each winding is on each limb, so the ampere-turns per limb are IHVTHV/2I_{HV}T_{HV}/2. KK = 0.75 assumed (single-phase core type), ρ=0.021 Ω\rho = 0.021\ \Omega-mm²/m. Winding data are given: LV 255/293 mm (inside/outside diameter), HV 314/351 mm, radial depths b1b_1 = 14 mm, b2b_2 = 18 mm, gap aa = 11 mm. Axial length taken as the mean of 268 and 276 mm, LcL_c = 272 mm.

i) Dimensions of core, window and yoke

Voltage per turn, Et=KQE_t = K\sqrt{Q} (QQ in kVA):

Et=0.75125=8.385 Vϕm=Et4.44f=8.3854.44×50=0.03777 WbAi=ϕmBm=0.037771.35=0.02798 m2=279.8 cm2\begin{aligned} E_t &= 0.75\sqrt{125} = 8.385\ \text{V}\\ \phi_m &= \frac{E_t}{4.44f} = \frac{8.385}{4.44\times50} = 0.03777\ \text{Wb}\\ A_i &= \frac{\phi_m}{B_m} = \frac{0.03777}{1.35} = 0.02798\ \text{m}^2 = 279.8\ \text{cm}^2 \end{aligned}

For a cruciform (two-stepped) core with stacking factor 0.9, Ai=0.56d2A_i = 0.56d^2 (standard ratio, Sawhney):

d=Ai0.56=0.027980.56=0.2235 m=223.5 mma=0.85d=190.0 mmb=0.53d=118.5 mm\begin{aligned} d &= \sqrt{\frac{A_i}{0.56}} = \sqrt{\frac{0.02798}{0.56}} = 0.2235\ \text{m} = 223.5\ \text{mm}\\ a &= 0.85d = 190.0\ \text{mm}\\ b &= 0.53d = 118.5\ \text{mm} \end{aligned}

Gross core area Agi=Ai/0.9=0.03109A_{gi} = A_i/0.9 = 0.03109 m².

Output equation (single phase): Q=2.22fBmδKwAwAi×10−3Q = 2.22fB_m\delta K_wA_wA_i\times10^{-3}

Aw=Q2.22fBmδKwAi×10−3=1252.22×50×1.35×2.75×106×0.3×0.02798×10−3=0.03614 m2Ww=Aw2.5=120.2 mm,Hw=2.5Ww=300.6 mmD=d+Ww=343.8 mm (distance between adjacent limb centres)\begin{aligned} A_w &= \frac{Q}{2.22fB_m\delta K_wA_i\times10^{-3}}\\ &= \frac{125}{2.22\times50\times1.35\times2.75\times10^6\times0.3\times0.02798\times10^{-3}}\\ &= 0.03614\ \text{m}^2\\ W_w &= \sqrt{\frac{A_w}{2.5}} = 120.2\ \text{mm},\quad H_w = 2.5W_w = 300.6\ \text{mm}\\ D &= d + W_w = 343.8\ \text{mm (distance between adjacent limb centres)} \end{aligned}

Check: dd = 224 mm fits inside the LV (255 mm) and coil height 276 mm < HwH_w. But HV outside diameter 351 mm > DD = 344 mm, so the window is widened (10 mm between the HV coils on the two limbs):

D=351+10=361 mm,Ww=D−d=137.5 mm,Hw=300.6 mm\begin{aligned} D &= 351 + 10 = 361\ \text{mm},\quad W_w = D - d = 137.5\ \text{mm},\quad H_w = 300.6\ \text{mm} \end{aligned}

Yoke:

Yoke area 20% more than core area (hot-rolled steel, to reduce yoke loss and magnetising current). Yoke depth = width of largest stamping:

Ay=1.2Ai=0.03357 m2,Agy=Ay0.9=0.03731 m2Dy=a=190.0 mmHy=AgyDy=0.037310.1900=196.3 mm\begin{aligned} A_y &= 1.2A_i = 0.03357\ \text{m}^2,\quad A_{gy} = \frac{A_y}{0.9} = 0.03731\ \text{m}^2\\ D_y &= a = 190.0\ \text{mm}\\ H_y &= \frac{A_{gy}}{D_y} = \frac{0.03731}{0.1900} = 196.3\ \text{mm} \end{aligned}

ii) Overall dimensions of frame

H=Hw+2Hy=300.6+2(196.3)=693.3 mmW=D+a=361.0+190.0=551.0 mmDepth=Dy=a=190.0 mm\begin{aligned} H &= H_w + 2H_y = 300.6 + 2(196.3) = 693.3\ \text{mm}\\ W &= D + a = 361.0 + 190.0 = 551.0\ \text{mm}\\ \text{Depth} &= D_y = a = 190.0\ \text{mm} \end{aligned}
 +-----------------------+  ---
 |       top yoke        |   ^
 +-----+-----------+-----+   |
 |limb |  window   |limb |   H
 |     |  Ww x Hw  |     |   |
 +-----+-----------+-----+   |
 |      bottom yoke      |   v
 +-----------------------+  ---
 |<--------- W --------->|
    |<----- D ----->|

iii) Leakage reactance

Currents: ILV=QVLV=312.50I_{LV} = \frac{Q}{V_{LV}} = 312.50 A; IHV=18.939I_{HV} = 18.939 A.

TLV=VLVEt=400.08.385=47.70≈48Et (revised)=400.048=8.333 VTHV=TLVVHVVLV=792.0≈792aLV=ILVδ=113.64 mm2,aHV=IHVδHV=6.887 mm2\begin{aligned} T_{LV} &= \frac{V_{LV}}{E_t} = \frac{400.0}{8.385} = 47.70 \approx 48\\ E_t\ (\text{revised}) &= \frac{400.0}{48} = 8.333\ \text{V}\\ T_{HV} &= T_{LV}\frac{V_{HV}}{V_{LV}} = 792.0 \approx 792\\ a_{LV} &= \frac{I_{LV}}{\delta} = 113.64\ \text{mm}^2,\quad a_{HV} = \frac{I_{HV}}{\delta_{HV}} = 6.887\ \text{mm}^2 \end{aligned}

Radial depths: b1=14b_1 = 14 mm (LV), b2=18b_2 = 18 mm (HV), duct a=11a = 11 mm.

Mean lengths of turn:

Lmt,LV=π255.0+293.02=0.8608 mLmt,HV=π314.0+351.02=1.0446 mLmt=π255.0+351.02=0.9519 m (both windings, for reactance)\begin{aligned} L_{mt,LV} &= \pi\frac{255.0 + 293.0}{2} = 0.8608\ \text{m}\\ L_{mt,HV} &= \pi\frac{314.0 + 351.0}{2} = 1.0446\ \text{m}\\ L_{mt} &= \pi\frac{255.0 + 351.0}{2} = 0.9519\ \text{m (both windings, for reactance)} \end{aligned}

Leakage reactance (per unit), with ATAT per limb =7500= 7500 and axial winding length Lc=272.0L_c = 272.0 mm:

εx=2πfμ0ATLc⋅LmtEt(a+b1+b23)=2π(50)(4π×10−7)75000.2720⋅0.95198.333(11+14+183)×10−3=0.0269 p.u.XHV=εxVHVIHV=0.0269×6600.018.94=9.388 Ω (referred to HV)XLV=XHV(TLVTHV)2=0.03448 Ω\begin{aligned} \varepsilon_x &= 2\pi f\mu_0\frac{AT}{L_c}\cdot\frac{L_{mt}}{E_t}\left(a + \frac{b_1+b_2}{3}\right)\\ &= 2\pi(50)(4\pi\times10^{-7})\frac{7500}{0.2720}\cdot\frac{0.9519}{8.333}\left(11 + \frac{14+18}{3}\right)\times10^{-3}\\ &= 0.0269\ \text{p.u.}\\ X_{HV} &= \varepsilon_x\frac{V_{HV}}{I_{HV}} = 0.0269\times\frac{6600.0}{18.94} = 9.388\ \Omega\ \text{(referred to HV)}\\ X_{LV} &= X_{HV}\left(\frac{T_{LV}}{T_{HV}}\right)^2 = 0.03448\ \Omega \end{aligned}

Answer: dd = 224 mm; window 137 × 301 mm; yoke 196 × 190 mm; frame 693 × 551 × 190 mm; leakage reactance ≈ 9.39 Ω referred to HV (2.69%).

✓ Answer checked by Claude Sonnet 5.5

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