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Design: 500 kVA 66/11 kV power transformer

Short answer

Cruciform core d=260 mm, stampings 221×138 mm; window 853 mm high × 310 mm wide; yoke depth 221 mm, height 228 mm; overall frame 1309×1360×221 mm. Per unit resistance drop 0.010, leakage reactance drop 0.065, voltage regulation at 0.8 pf lagging 0.0472 (4.72%).

For a 500 kVA, 3-phase, 50 Hz, 66/11 kV, delta/star, core type, oil immersed natural cooled power transformer the design data are: Maximum flux density in the core = 1.6 Wb/m²; Constant for output voltage per turn = 0.6; Core type = cruciform; Current density in the conductor = 2.5 A/mm²; Window space factor = 0.22; Stacking factor = 0.9; Ratio of window height to width = 2.75. Width of duct between LV and core, LV winding, HV winding and duct between HV and LV are 10 mm, 50 mm, 60 mm, 20 mm respectively. Assuming all other required parameters, calculate: (i) Overall dimension of core (ii) Overall dimension of frame (iii) Per unit resistance and leakage reactance drop (iv) Per unit voltage regulation

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: yoke area 1.2 × core area (hot-rolled steel), end clearance 50 mm (66 kV), ρ=0.021 Ω\rho = 0.021\ \Omega-mm²/m, regulation at 0.8 pf lagging (pf not given).

(i) Overall dimensions of core

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

Et=0.6500=13.416 Vϕm=Et4.44f=13.4164.44×50=0.06043 WbAi=ϕmBm=0.060431.6=0.03777 m2=377.7 cm2\begin{aligned} E_t &= 0.6\sqrt{500} = 13.416\ \text{V}\\ \phi_m &= \frac{E_t}{4.44f} = \frac{13.416}{4.44\times50} = 0.06043\ \text{Wb}\\ A_i &= \frac{\phi_m}{B_m} = \frac{0.06043}{1.6} = 0.03777\ \text{m}^2 = 377.7\ \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=0.037770.56=0.2597 m=259.7 mma=0.85d=220.8 mmb=0.53d=137.6 mm\begin{aligned} d &= \sqrt{\frac{A_i}{0.56}} = \sqrt{\frac{0.03777}{0.56}} = 0.2597\ \text{m} = 259.7\ \text{mm}\\ a &= 0.85d = 220.8\ \text{mm}\\ b &= 0.53d = 137.6\ \text{mm} \end{aligned}

Gross core area Agi=Ai/0.9=0.04197A_{gi} = A_i/0.9 = 0.04197 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=5003.33×50×1.6×2.5×106×0.22×0.03777×10−3=0.09035 m2Ww=Aw2.75=181.3 mm,Hw=2.75Ww=498.4 mmD=d+Ww=441.0 mm (distance between adjacent limb centres)\begin{aligned} A_w &= \frac{Q}{3.33fB_m\delta K_wA_i\times10^{-3}}\\ &= \frac{500}{3.33\times50\times1.6\times2.5\times10^6\times0.22\times0.03777\times10^{-3}}\\ &= 0.09035\ \text{m}^2\\ W_w &= \sqrt{\frac{A_w}{2.75}} = 181.3\ \text{mm},\quad H_w = 2.75W_w = 498.4\ \text{mm}\\ D &= d + W_w = 441.0\ \text{mm (distance between adjacent limb centres)} \end{aligned}

Winding build (LV next to core):

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

ItemInside dia (mm)Outside dia (mm)
LV winding279.7379.7
HV winding419.7539.7

Radial depths: b1=50b_1 = 50 mm (LV), b2=60b_2 = 60 mm (HV), duct a=20a = 20 mm. Axial length of coil, from the output-equation window height: Lc=Hw−2(50)=398.4L_c = H_w - 2(50) = 398.4 mm.

Mean lengths of turn:

Lmt,LV=π279.7+379.72=1.0358 mLmt,HV=π419.7+539.72=1.5071 mLmt=π279.7+539.72=1.2871 m (both windings, for reactance)\begin{aligned} L_{mt,LV} &= \pi\frac{279.7 + 379.7}{2} = 1.0358\ \text{m}\\ L_{mt,HV} &= \pi\frac{419.7 + 539.7}{2} = 1.5071\ \text{m}\\ L_{mt} &= \pi\frac{279.7 + 539.7}{2} = 1.2871\ \text{m (both windings, for reactance)} \end{aligned}

Check: the HV outside diameter is 539.7 mm but DD from the output equation is only 441.0 mm, so the coils of adjacent limbs would overlap. The window is widened so that there is 30 mm clearance between adjacent HV coils (66 kV), and its height is increased to keep the given ratio Hw/Ww=2.75H_w/W_w = 2.75. The coil height stays at LcL_c = 398.4 mm.

D=do,HV+30=569.7 mmWw=D−d=310.0 mm,Hw=2.75Ww=852.5 mm\begin{aligned} D &= d_{o,HV} + 30 = 569.7\ \text{mm}\\ W_w &= D - d = 310.0\ \text{mm},\quad H_w = 2.75W_w = 852.5\ \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=0.04533 m2,Agy=Ay0.9=0.05036 m2Dy=a=220.8 mmHy=AgyDy=0.050360.2208=228.1 mm\begin{aligned} A_y &= 1.2A_i = 0.04533\ \text{m}^2,\quad A_{gy} = \frac{A_y}{0.9} = 0.05036\ \text{m}^2\\ D_y &= a = 220.8\ \text{mm}\\ H_y &= \frac{A_{gy}}{D_y} = \frac{0.05036}{0.2208} = 228.1\ \text{mm} \end{aligned}

(ii) Overall dimensions of frame

H=Hw+2Hy=852.5+2(228.1)=1308.8 mmW=2D+a=2(569.7)+220.8=1360.2 mmDepth=Dy=a=220.8 mm\begin{aligned} H &= H_w + 2H_y = 852.5 + 2(228.1) = 1308.8\ \text{mm}\\ W &= 2D + a = 2(569.7) + 220.8 = 1360.2\ \text{mm}\\ \text{Depth} &= D_y = a = 220.8\ \text{mm} \end{aligned}
 +-----------------------------+  ---
 |          top yoke           |   ^
 +-----+-----+-----+-----+-----+   |
 |limb |     |limb |     |limb |   |
 |  R  | Ww  |  Y  | Ww  |  B  |   H
 |     |     |     |     |     |   |
 +-----+-----+-----+-----+-----+   |
 |         bottom yoke         |   v
 +-----------------------------+  ---
 |<------------ W ------------>|
    |<--- D --->|<--- D --->|

(iii) Per unit resistance and leakage reactance drop

Phase voltages: LV (star) VLV=6350.9V_{LV} = 6350.9 V; HV (delta) VHV=66000.0V_{HV} = 66000.0 V.

Phase currents: ILV=Q3VLV=26.24I_{LV} = \frac{Q}{3V_{LV}} = 26.24 A; IHV=2.525I_{HV} = 2.525 A.

TLV=VLVEt=6350.913.416=473.36≈473Et (revised)=6350.9473=13.427 VTHV=TLVVHVVLV=4915.6≈4916aLV=ILVδ=10.50 mm2,aHV=IHVδHV=1.010 mm2\begin{aligned} T_{LV} &= \frac{V_{LV}}{E_t} = \frac{6350.9}{13.416} = 473.36 \approx 473\\ E_t\ (\text{revised}) &= \frac{6350.9}{473} = 13.427\ \text{V}\\ T_{HV} &= T_{LV}\frac{V_{HV}}{V_{LV}} = 4915.6 \approx 4916\\ a_{LV} &= \frac{I_{LV}}{\delta} = 10.50\ \text{mm}^2,\quad a_{HV} = \frac{I_{HV}}{\delta_{HV}} = 1.010\ \text{mm}^2 \end{aligned}

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=0.021×4916×1.50711.010=154.03 ΩrLV=0.021×473×1.035810.50=0.98013 ΩRp=rHV+rLV(THVTLV)2=154.03+0.98013(4916473)2=259.9 Ωεr=IHVRpVHV=2.525×259.966000.0=0.00994 p.u.\begin{aligned} r_{HV} &= \frac{\rho T_{HV}L_{mt,HV}}{a_{HV}} = \frac{0.021\times4916\times1.5071}{1.010} = 154.03\ \Omega\\ r_{LV} &= \frac{0.021\times473\times1.0358}{10.50} = 0.98013\ \Omega\\ R_p &= r_{HV} + r_{LV}\left(\frac{T_{HV}}{T_{LV}}\right)^2 = 154.03 + 0.98013\left(\frac{4916}{473}\right)^2 = 259.9\ \Omega\\ \varepsilon_r &= \frac{I_{HV}R_p}{V_{HV}} = \frac{2.525\times259.9}{66000.0} = 0.00994\ \text{p.u.} \end{aligned}

Leakage reactance (per unit), with ATAT per limb =12414= 12414 and axial winding length Lc=398.4L_c = 398.4 mm:

εx=2πfμ0ATLc⋅LmtEt(a+b1+b23)=2π(50)(4π×10−7)124140.3984⋅1.287113.427(20+50+603)×10−3=0.0668 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{12414}{0.3984}\cdot\frac{1.2871}{13.427}\left(20 + \frac{50+60}{3}\right)\times10^{-3}\\ &= 0.0668\ \text{p.u.} \end{aligned}

(iv) Per unit voltage regulation (0.8 pf lagging)

ε=εrcos⁡ϕ+εxsin⁡ϕ=0.00994(0.8)+0.0668(0.600)=0.0480 p.u.=4.80%\begin{aligned} \varepsilon &= \varepsilon_r\cos\phi + \varepsilon_x\sin\phi\\ &= 0.00994(0.8) + 0.0668(0.600) = 0.0480\ \text{p.u.} = 4.80\% \end{aligned}

Answer: dd = 260 mm; window 310 × 853 mm (after widening); frame 1309 × 1360 × 221 mm; εr\varepsilon_r = 0.0099, εx\varepsilon_x = 0.0668; regulation ≈ 4.80%.

✓ Answer checked by Claude Sonnet 5.5

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