Solutions Pdf | Magnetic Circuits Problems And

Given: After fault, (\Phi_actual = 0.8\ \textmWb) at (NI=250). So total reluctance = (250 / 0.8\times10^-3 = 312.5 \ \textkA-t/Wb). Core reluctance alone = (497.4 \ \textkA-t/Wb). If total reluctance is lower than iron alone, that’s impossible. Therefore: The original core for design purposes. The fault increased the gap.

Let’s find gap length that gives (\mathcalR total = 312.5\ \textkA-t/Wb): [ \mathcalR g = \mathcalR total - \mathcalR iron = 312.5 - 497.4 = -184.9 \ \text(negative → impossible) ] Conclusion: The core is saturating or the permeability has dropped. A better problem would give (\Phi_healthy) first. magnetic circuits problems and solutions pdf

Reluctance without gap: [ \mathcalR c,iron = \frac0.15(4\pi\times 10^-7)(600)(4\times 10^-4) \approx 497.4 \ \textkA-t/Wb ] MMF = (\Phi \mathcalR) → (250 = (1.2\times 10^-3) \times \mathcalR total,des ) So (\mathcalR_total,des \approx 208.3 \ \textkA-t/Wb) – but that’s than iron reluctance alone? That’s impossible. Given: After fault, (\Phi_actual = 0

Center limb: [ \mathcalR_c = \frac0.1(4\pi\times 10^-7)(1000)(6\times 10^-4) \approx 132.6 \ \textkA-t/Wb ] Each outer limb: [ \mathcalR_o = \frac0.2(4\pi\times 10^-7)(1000)(3\times 10^-4) \approx 530.5 \ \textkA-t/Wb ] Yoke (each, two yokes in series effectively for each flux path): [ \mathcalR y = \frac0.05(4\pi\times 10^-7)(1000)(6\times 10^-4) \approx 66.3 \ \textkA-t/Wb ] Total for one outer path (center → yoke → outer limb → yoke → center): [ \mathcalR outer, total = \mathcalR_c + 2\mathcalR_y + \mathcalR_o ] [ = 132.6 + 2(66.3) + 530.5 = 795.7 \ \textkA-t/Wb ] But careful: The two outer paths are after the center limb. If total reluctance is lower than iron alone,

So: [ \mathcalR_eq, branches = \frac(\mathcalR_o + 2\mathcalR_y)2 = \frac530.5 + 132.62 = 331.55 \ \textkA-t/Wb ] Wait – (2\mathcalR_y = 132.6), so (\mathcalR_o + 2\mathcalR_y = 530.5+132.6 = 663.1). Half of that is kA-t/Wb.