Question 5 of 7: Magnetic Circuit — MMF, Reluctance and Air-Gap Flux
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
04-BS-4 Electric Circuits and Power — December 2017
National Exams, 3 hours, closed book (one aid sheet permitted). Any five of the seven questions constitute a complete paper; all seven are solved below as a complete study resource.
Reference texts
Sadiku, C.K. Alexander & M.N.O. Sadiku, Fundamentals of Electric Circuits — DC/AC circuit analysis, Thevenin theorem, magnetic circuits (Ch. 13).
S. Chapman, Electric Machinery Fundamentals — magnetic circuits and reluctance.
R. Boylestad, Electronic Devices and Circuit Theory — diode rectifiers and RC filters.
M.M. Mano, Digital Design — combinational logic design.
Question 5: Magnetic Circuit — MMF, Reluctance and Air-Gap Flux (20 marks)
Given. Double-window (two-window, E-I style) core: the coil ($N$ turns) is wound on the centre leg; a 0.2 mm air gap sits in the right outer leg only (the left outer leg is solid iron). All legs share the same uniform cross-section.
Given data
$A$
$\mu_r$
$N$
$I$
Leg height
Right leg iron
Gap $l_g$
100 mm²
2000
100
1 A
50 mm
49.8 mm
0.2 mm
Find. MMF; $\mathcal{R}_{center}$, $\mathcal{R}_{left}$, $\mathcal{R}_{right,iron}$, $\mathcal{R}_{gap}$; the analog circuit; $\Phi_{gap}$, $B_{gap}$, $H_{gap}$.
Figure 5: Magnetic core - coil on centre leg, 0.2 mm gap in right outer leg
Approach. Treat the core exactly like the DC bridge of Question 1: the coil-leg reluctance is a series element carrying the total flux, which then splits between the two outer legs (in parallel) back to the yoke. The left leg is all iron; the right leg is iron in series with the air gap.
a) Magnetomotive force. $$\mathcal{F} = NI = (100)(1\text{ A}) = \boxed{100\text{ A-turns}}$$
b) Reluctances. $\mathcal{R}=\dfrac{l}{\mu A}$, with $A=100\text{ mm}^2=1\times10^{-4}\text{ m}^2$. Centre and left legs share the same iron length (50 mm, no gap); the right leg splits into 49.8 mm of iron plus the 0.2 mm gap ($\mu_r=1$ in air):
$$\mathcal{R}_{center}=\mathcal{R}_{left}=\frac{0.050}{(4\pi\times10^{-7})(2000)(10^{-4})}=1.989\times10^{5}\text{ A-t/Wb}$$
$$\mathcal{R}_{right,iron}=\frac{0.0498}{(4\pi\times10^{-7})(2000)(10^{-4})}=1.981\times10^{5}\text{ A-t/Wb}$$
$$\mathcal{R}_{gap}=\frac{0.0002}{(4\pi\times10^{-7})(1)(10^{-4})}=\boxed{1.592\times10^{6}\text{ A-t/Wb}}$$
The 0.2 mm gap alone contributes 89% of the right leg's total reluctance ($\mathcal{R}_{right}=\mathcal{R}_{right,iron}+\mathcal{R}_{gap}=1.790\times10^6$), which is the usual signature of an air-gapped magnetic circuit.
c) Analog circuit. The MMF source drives $\mathcal{R}_{center}$ in series with the parallel combination of $\mathcal{R}_{left}$ and $(\mathcal{R}_{right,iron}+\mathcal{R}_{gap})$ — identical topology to the electrical bridge of Question 1, with MMF↔voltage, flux↔current, reluctance↔resistance.
Figure 5b: Reluctance-network analog of the magnetic circuit
d) Flux, flux density and field intensity in the gap.
$$\mathcal{R}_{par}=\mathcal{R}_{left}\parallel\mathcal{R}_{right}=1.790\times10^{5}\text{ A-t/Wb}\ ,\quad \mathcal{R}_{tot}=\mathcal{R}_{center}+\mathcal{R}_{par}=3.780\times10^{5}\text{ A-t/Wb}$$
$$\Phi_{total}=\frac{\mathcal{F}}{\mathcal{R}_{tot}}=\frac{100}{3.780\times10^{5}}=2.646\times10^{-4}\text{ Wb}$$
Current-divider analog splits $\Phi_{total}$ between the two outer legs; the gap carries the entire right-branch flux:
$$\Phi_{gap}=\Phi_{total}\cdot\frac{\mathcal{R}_{left}}{\mathcal{R}_{left}+\mathcal{R}_{right}}=\boxed{2.647\times10^{-5}\text{ Wb}}$$
$$B_{gap}=\frac{\Phi_{gap}}{A}=\frac{2.647\times10^{-5}}{1\times10^{-4}}=\boxed{0.2647\text{ T}}\ ,\qquad H_{gap}=\frac{B_{gap}}{\mu_0}=\boxed{2.106\times10^{5}\text{ A/m}}$$
Final results — Question 5
Quantity
Value
MMF
100 A-turns
$\mathcal{R}_{center}=\mathcal{R}_{left}$
1.989×105 A-t/Wb
$\mathcal{R}_{right,iron}$
1.981×105 A-t/Wb
$\mathcal{R}_{gap}$
1.592×106 A-t/Wb
$\Phi_{total}$
2.646×10-4 Wb
$\Phi_{gap}$
2.647×10-5 Wb
$B_{gap}$
0.2647 T
$H_{gap}$
2.106×105 A/m
Check: no separate yoke (top/bottom horizontal member) length is dimensioned in the figure, so each vertical leg's mean path is taken as the full 50 mm core height (matching the explicitly-dimensioned 24.9+0.2+24.9 mm on the right leg); the sub-mm air gap supplies ~80% of the total loop reluctance regardless, so this assumption barely moves $B_{gap}$/$H_{gap}$.