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Why iron loss neglected in SC test; parameters

Short answer

Short circuit test uses only 5–10% rated voltage, so flux and iron loss are negligible. Equivalent circuit parameters referred to primary (400 V): Req = 1.08 Ω, Xeq = 1.269 Ω, R0 = 1455 Ω, X0 = 573.3 Ω.

Why is iron loss neglected in short circuit test of transformer? A single phase 400/200 V, 50 Hz transformer gave the following test results: Open circuit Test: 200 V, 1.5 A, 110 W on LV side Short circuit Test: 30 V, 18 A, 350 W on HV side Calculate the equivalent circuit parameters referred to primary side and draw the equivalent circuit showing calculated parameters.

Why iron loss is neglected in the SC test

In the short-circuit test only a small voltage (about 5 to 10% of the rated value) is applied, just enough to circulate full-load current in the shorted secondary. The core flux is proportional to the applied voltage, so it is only about 5 to 10% of normal flux. Core loss varies approximately as the square of the flux, so it becomes about 0.25 to 1% of the rated core loss, which is negligible. The wattmeter therefore reads the copper loss alone. In this problem 30/400=7.5%30/400 = 7.5\% of rated voltage, so the core loss is about 0.0752×110≈0.60.075^2\times110 \approx 0.6 W against 350 W.

Equivalent circuit parameters (referred to the primary)

Primary = HV side (400 V), secondary = LV side (200 V).

Open-circuit test (on the LV side)

The no-load power is almost entirely core loss, so the shunt branch is found from it.

cos⁡ϕ0=P0V0I0=110200×1.5=0.3667Iw=I0cos⁡ϕ0=0.55 A,Iμ=I02−Iw2=1.396 AR0=V0Iw=363.6 Ω,X0=V0Iμ=143.3 Ω(on the LV side)\begin{aligned} \cos\phi_0 &= \frac{P_0}{V_0I_0} = \frac{110}{200\times1.5} = 0.3667 \\ I_w &= I_0\cos\phi_0 = 0.55\ \text{A},\qquad I_\mu = \sqrt{I_0^2 - I_w^2} = 1.396\ \text{A} \\ R_0 &= \frac{V_0}{I_w} = 363.6\ \Omega,\qquad X_0 = \frac{V_0}{I_\mu} = 143.3\ \Omega\quad(\text{on the LV side}) \end{aligned}

Short-circuit test (on the HV side)

At the reduced test voltage the core loss is negligible, so the wattmeter reading is the copper loss.

Zsc=VscIsc=3018=1.667 ΩRsc=PscIsc2=350182=1.08 ΩXsc=Zsc2−Rsc2=1.269 Ω(on the HV side)\begin{aligned} Z_{sc} &= \frac{V_{sc}}{I_{sc}} = \frac{30}{18} = 1.667\ \Omega \\ R_{sc} &= \frac{P_{sc}}{I_{sc}^2} = \frac{350}{18^2} = 1.08\ \Omega \\ X_{sc} &= \sqrt{Z_{sc}^2 - R_{sc}^2} = 1.269\ \Omega\quad(\text{on the HV side}) \end{aligned}

Referring to the HV side

The turns ratio is K=400/200=2K = 400/200 = 2, so K2=4K^2 = 4. Impedances are multiplied by K2K^2 when moved from LV to HV, and divided by K2K^2 when moved from HV to LV.

R0′=363.6×4=1455 ΩX0′=143.3×4=573.3 Ω\begin{aligned} R_0' &= 363.6 \times 4 = 1455\ \Omega \\ X_0' &= 143.3 \times 4 = 573.3\ \Omega \end{aligned}

Equivalent circuit referred to the HV side

   Req=1.08 ohm   Xeq=1.27 ohm
 o--+-----/\/\/\-----UUUU------o
    |                          
   [R0=1455] [X0=573.3]   Load
    |      (in parallel)
 o--+---------------------------o

Req=1.08 ΩR_{eq} = 1.08\ \Omega, Xeq=1.269 ΩX_{eq} = 1.269\ \Omega (Zeq=1.667 ΩZ_{eq} = 1.667\ \Omega), shunt branch R0=1455 ΩR_0 = 1455\ \Omega in parallel with X0=573.3 ΩX_0 = 573.3\ \Omega.

The shunt branch carries I0I_0 referred to the primary =1.5/2=0.75= 1.5/2 = 0.75 A.

Answer (referred to primary): R01=1.080 ΩR_{01} = 1.080\ \Omega, X01=1.269 ΩX_{01} = 1.269\ \Omega, R0=1454.5 ΩR_0 = 1454.5\ \Omega, X0=573.3 ΩX_0 = 573.3\ \Omega.

✓ Answer checked by Claude Opus 5.5 (high effort)

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