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Design data: 1000 kVA 66/11 kV transformer

Short answer

Core d=324.4 mm, cruciform (a=275.8, b=171.9 mm); window 267.4×735.2 mm; yoke depth 275.8 mm height 285.0 mm; frame H=1305.2 mm, W=1459.3 mm, depth 275.8 mm.

The design parameters for a 1000 kVA, 50 Hz, 66/11 kV, 3-phase, delta/delta, core type, oil immersed natural cooled power transformer are given below. Constant for output voltage per turn = 0.6; Maximum flux density in the core = 1.45 Wb/m²; Current density in conductor = 2.75 A/mm²; Core type = cruciform two stepped; Window space factor = 0.13; Stacking factor = 0.9; Ratio of window height to width = 2.75; Take hot rolled steel and area of yoke is 20% greater than gross area of core; Width of LV winding = 40 mm; Width of HV winding = 50 mm; Width of duct between HV and LV winding = 20 mm; Resistivity of copper = 0.021 Ω-mm²/m. [The list of quantities to calculate is not shown in the scanned paper.]

The list of quantities is missing from the paper, so the usual set is worked out: core, window and yoke; overall frame; per unit resistance and reactance; regulation at 0.8 pf lagging. 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. Assumed: core-to-LV clearance 10 mm, end clearance 50 mm (66 kV), ρ=0.021 Ω\rho = 0.021\ \Omega-mm²/m.

Core and window

Voltage per turn, Et=KQE_t = K\sqrt{Q} (QQ in kVA, total for 3 phases):

Et=0.61000=18.974 Vϕm=Et4.44f=18.9744.44×50=0.08547 WbAi=ϕmBm=0.085471.45=0.05894 m2=589.4 cm2\begin{aligned} E_t &= 0.6\sqrt{1000} = 18.974\ \text{V}\\ \phi_m &= \frac{E_t}{4.44f} = \frac{18.974}{4.44\times50} = 0.08547\ \text{Wb}\\ A_i &= \frac{\phi_m}{B_m} = \frac{0.08547}{1.45} = 0.05894\ \text{m}^2 = 589.4\ \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=0.058940.56=0.3244 m=324.4 mma=0.85d=275.8 mmb=0.53d=171.9 mm\begin{aligned} d &= \sqrt{\frac{A_i}{0.56}} = \sqrt{\frac{0.05894}{0.56}} = 0.3244\ \text{m} = 324.4\ \text{mm}\\ a &= 0.85d = 275.8\ \text{mm}\\ b &= 0.53d = 171.9\ \text{mm} \end{aligned}

Gross core area Agi=Ai/0.9=0.06549A_{gi} = A_i/0.9 = 0.06549 m².

Output equation (three phase): Q=3.33fBmδKwAwAi×10−3Q = 3.33fB_m\delta K_wA_wA_i\times10^{-3}

Aw=Q3.33fBmδKwAi×10−3=10003.33×50×1.45×2.75×106×0.13×0.05894×10−3=0.19657 m2Ww=Aw2.75=267.4 mm,Hw=2.75Ww=735.2 mmD=d+Ww=591.8 mm (distance between adjacent limb centres)\begin{aligned} A_w &= \frac{Q}{3.33fB_m\delta K_wA_i\times10^{-3}}\\ &= \frac{1000}{3.33\times50\times1.45\times2.75\times10^6\times0.13\times0.05894\times10^{-3}}\\ &= 0.19657\ \text{m}^2\\ W_w &= \sqrt{\frac{A_w}{2.75}} = 267.4\ \text{mm},\quad H_w = 2.75W_w = 735.2\ \text{mm}\\ D &= d + W_w = 591.8\ \text{mm (distance between adjacent limb centres)} \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=0.07073 m2,Agy=Ay0.9=0.07859 m2Dy=a=275.8 mmHy=AgyDy=0.078590.2758=285.0 mm\begin{aligned} A_y &= 1.2A_i = 0.07073\ \text{m}^2,\quad A_{gy} = \frac{A_y}{0.9} = 0.07859\ \text{m}^2\\ D_y &= a = 275.8\ \text{mm}\\ H_y &= \frac{A_{gy}}{D_y} = \frac{0.07859}{0.2758} = 285.0\ \text{mm} \end{aligned}

Overall dimensions of frame

H=Hw+2Hy=735.2+2(285.0)=1305.2 mmW=2D+a=2(591.8)+275.8=1459.3 mmDepth=Dy=a=275.8 mm\begin{aligned} H &= H_w + 2H_y = 735.2 + 2(285.0) = 1305.2\ \text{mm}\\ W &= 2D + a = 2(591.8) + 275.8 = 1459.3\ \text{mm}\\ \text{Depth} &= D_y = a = 275.8\ \text{mm} \end{aligned}
 +-----------------------------+  ---
 |          top yoke           |   ^
 +-----+-----+-----+-----+-----+   |
 |limb |     |limb |     |limb |   |
 |  R  | Ww  |  Y  | Ww  |  B  |   H
 |     |     |     |     |     |   |
 +-----+-----+-----+-----+-----+   |
 |         bottom yoke         |   v
 +-----------------------------+  ---
 |<------------ W ------------>|
    |<--- D --->|<--- D --->|

Turns and conductors (delta/delta)

Phase voltages: LV (delta) VLV=11000.0V_{LV} = 11000.0 V; HV (delta) VHV=66000.0V_{HV} = 66000.0 V.

Phase currents: ILV=Q3VLV=30.30I_{LV} = \frac{Q}{3V_{LV}} = 30.30 A; IHV=5.051I_{HV} = 5.051 A.

TLV=VLVEt=11000.018.974=579.75≈580Et (revised)=11000.0580=18.966 VTHV=TLVVHVVLV=3480.0≈3480aLV=ILVδ=11.02 mm2,aHV=IHVδHV=1.837 mm2\begin{aligned} T_{LV} &= \frac{V_{LV}}{E_t} = \frac{11000.0}{18.974} = 579.75 \approx 580\\ E_t\ (\text{revised}) &= \frac{11000.0}{580} = 18.966\ \text{V}\\ T_{HV} &= T_{LV}\frac{V_{HV}}{V_{LV}} = 3480.0 \approx 3480\\ a_{LV} &= \frac{I_{LV}}{\delta} = 11.02\ \text{mm}^2,\quad a_{HV} = \frac{I_{HV}}{\delta_{HV}} = 1.837\ \text{mm}^2 \end{aligned}

Winding dimensions

Radial build (assumed clearance between core and LV = 10 mm):

ItemInside dia (mm)Outside dia (mm)
LV winding344.4424.4
HV winding464.4564.4

Radial depths: b1=40b_1 = 40 mm (LV), b2=50b_2 = 50 mm (HV), duct a=20a = 20 mm. Axial length Lc=Hw−2(50)=635.2L_c = H_w - 2(50) = 635.2 mm.

Mean lengths of turn:

Lmt,LV=π344.4+424.42=1.2077 mLmt,HV=π464.4+564.42=1.6161 mLmt=π344.4+564.42=1.4276 m (both windings, for reactance)\begin{aligned} L_{mt,LV} &= \pi\frac{344.4 + 424.4}{2} = 1.2077\ \text{m}\\ L_{mt,HV} &= \pi\frac{464.4 + 564.4}{2} = 1.6161\ \text{m}\\ L_{mt} &= \pi\frac{344.4 + 564.4}{2} = 1.4276\ \text{m (both windings, for reactance)} \end{aligned}

Check: HV outside diameter 564 mm vs DD = 592 mm. Adjacent HV coils have about 27 mm clearance, so the coils fit.

Per unit resistance

Resistance referred to HV, with ρ=0.021 Ω-mm2/m\rho = 0.021\ \Omega\text{-mm}^2/\text{m} (copper at about 75 °C):

rHV=ρTHVLmt,HVaHV=0.021×3480×1.61611.837=64.309 ΩrLV=0.021×580×1.207711.02=1.3349 ΩRp=rHV+rLV(THVTLV)2=64.309+1.3349(3480580)2=112.37 Ωεr=IHVRpVHV=5.051×112.3766000.0=0.00860 p.u.\begin{aligned} r_{HV} &= \frac{\rho T_{HV}L_{mt,HV}}{a_{HV}} = \frac{0.021\times3480\times1.6161}{1.837} = 64.309\ \Omega\\ r_{LV} &= \frac{0.021\times580\times1.2077}{11.02} = 1.3349\ \Omega\\ R_p &= r_{HV} + r_{LV}\left(\frac{T_{HV}}{T_{LV}}\right)^2 = 64.309 + 1.3349\left(\frac{3480}{580}\right)^2 = 112.37\ \Omega\\ \varepsilon_r &= \frac{I_{HV}R_p}{V_{HV}} = \frac{5.051\times112.37}{66000.0} = 0.00860\ \text{p.u.} \end{aligned}

Per unit leakage reactance

Leakage reactance (per unit), with ATAT per limb =17576= 17576 and axial winding length Lc=635.2L_c = 635.2 mm:

εx=2πfμ0ATLc⋅LmtEt(a+b1+b23)=2π(50)(4π×10−7)175760.6352⋅1.427618.966(20+40+503)×10−3=0.0411 p.u.\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{17576}{0.6352}\cdot\frac{1.4276}{18.966}\left(20 + \frac{40+50}{3}\right)\times10^{-3}\\ &= 0.0411\ \text{p.u.} \end{aligned}

Regulation at 0.8 pf lagging

ε=εrcos⁡ϕ+εxsin⁡ϕ=0.00860(0.8)+0.0411(0.600)=0.0315 p.u.=3.15%\begin{aligned} \varepsilon &= \varepsilon_r\cos\phi + \varepsilon_x\sin\phi\\ &= 0.00860(0.8) + 0.0411(0.600) = 0.0315\ \text{p.u.} = 3.15\% \end{aligned}

Answer: dd = 324 mm; window 267 × 735 mm; frame 1305 × 1459 × 276 mm; εr\varepsilon_r = 0.0086, εx\varepsilon_x = 0.0411; regulation ≈ 3.15%.

✓ Answer checked by Claude Sonnet 5.5

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