1Strand geometry
R_active = 0.2396 mΩ
2Parallel strands & positionsHow many electrically-parallel strands share the bundle current, and where each sits within the slot's conductor stack (0 = slot bottom, 1 = slot top). Strands at very different positions see very different slot-leakage field, driving circulating current between them.
0
0.33
0.67
1
3Slot & duty
Results
Total loss
46W
2.88× the ideal equal-sharing loss
Added circulating loss
30W
on top of 16 W ideal
Max circulating current
221.2A
of 100 A ideal share/strand
StrandPosition ξCurrent (A)Circulating (A)
s10310.6221.2
s20.33124.751.6
s30.6748.497.1
s4127.1118.7
Reference & assumptions

New to Slot-Leakage Loop Inductance (Classical Machine Design)? Read the guide: Parallel Path Circulating Current: Why Untransposed Strands Fight Each Other — a plain-language explainer of the standard behind this calculator.

Circulating current arises when electrically-parallel strands sit at different depths within a slot: the slot-leakage field builds up with depth, so each strand links a different amount of flux, and because the strands are joined at both ends the resulting EMF difference drives current around the loop between them — on top of, not instead of, the useful bundle current. This calculator solves the N strands as a coupled network (every strand at the same terminal voltage, currents summing to the bundle current) using the classical slot-leakage loop inductance between two strand positions, Lloop = (μ₀·lactive/bslot)·|yj−yk| — a thin-strand approximation cross-verified this session against the modern hairpin-winding literature, classical transformer leakage theory, and an independent first-principles energy derivation. The thin-strand approximation over-predicts (conservatively) circulating current for strands whose height is comparable to their separation — a finite-conductor-height correction is not applied. The model assumes the strands shown are the slot's full conductor content (other, non-parallel turns sharing the same slot are not separately modelled); 2-D/3-D field fringing, iron saturation, and end-region leakage are also not modelled. Transposition is modelled as each strand's length-averaged position — a simplification of the true continuous effect. No external absolute-watt worked example exists in the literature for this exact configuration, so validation here is structural (zero circulating current for identical positions or ideal transposition, current-deviation conservation, loss never decreasing) plus a self-consistent hand-derived numeric case. Verify against FEA before relying on absolute magnitudes for a final design.

Validated: a closed-form 2-strand solution hand-derived from this same model, Iδ = [jω·Lloop·Ibundle/2] / [2R+jω·Lloop], reproduces this calculator's output to 4 significant figures. Strands at the same position, or under ideal transposition, give exactly zero circulating current; swapping two strands' positions leaves total loss unchanged; current deviations from the ideal share always sum to zero; total loss never falls below the ideal equal-sharing loss.

Calculation steps
1. Slot-leakage loop inductance (per strand pair)
L_loop,jk = (μ0·l_active/b_slot)·|y_j − y_k| (thin-strand slot-leakage permeance)
l_active = 150 mm, b_slot = 8 mm, stack height = 15 mm
4 strands solved as a coupled network (self + mutual inductance matrix)
2. Coupled network solve
R_j·I_j + jω·Σ_k L_jk·I_k = V_common (same ∀j), Σ_j I_j = I_bundle
R_strand = 0.2396 mΩ (active) × α_w, f = 800 Hz
max circulating current = 221.2 A
3. Loss
P_ideal = ΣR_j·(I_bundle/N)², P_total = ΣR_j·|I_j|², P_added = P_total − P_ideal
I_bundle = 400 A RMS, N = 4 strands
P_ideal = 15.97 W, P_added = 30 W, total = 45.97 W (2.88×)