NivaarExam PrepOfficial exam papers ↗

22-Elec-A6 Power Systems and Machines · Undated paper

Question 1 of 5: Magnetic Circuit of a Toroid

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format: Closed-book, 3 hours. Five questions constitute a complete paper and all are of equal value (20 marks each); answer all five. All AC voltages and currents are rms, three-phase voltages are line-to-line, and power is total real power unless noted otherwise.

Reference texts (22-Elec-A6 Power Systems and Machines): S. J. Chapman, Electric Machinery Fundamentals, 5th ed. (McGraw-Hill); B. S. Guru & H. R. Hiziroglu, Electric Machinery and Transformers, 3rd ed. (Oxford); P. C. Sen, Principles of Electric Machines and Power Electronics, 2nd ed. (Wiley).

Note — paper identity. This paper’s own running header reads 16-Elec-A6/May 2019, so it is the May 2019 sitting. Question 2’s closing assumption is printed as "losses are too small to account for"; the reading adopted below is that the core losses are too small to account for (see the note under Question 2).

Question 1: Magnetic Circuit of a Toroid (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. A toroidal iron core wound with a magnetizing coil carrying DC.

Given data
Mean radius$r_{av} = 25\ \text{cm} = 0.25\ \text{m}$
Cross-sectional area$A = 3\ \text{cm}^2 = 3\times10^{-4}\ \text{m}^2$
Number of turns$N = 600$
Coil current$I = 1.5\ \text{A}$
Relative permeability$\mu_r = 1500$

[Figure not reproduced: Figure 1 (redrawn): partially wound toroid; the dashed line is the mean magnetic path of length $\ell = 2\pi r_{av}$, and the flux density $B$ circulates around it. See the official exam paper.]

Find. The circuit reluctance $\mathcal{R}$, the magnetomotive force $\mathcal{F}$ and field intensity $H$, and the flux $\Phi$ and flux density $B$.

Approach. Treat the toroid as a single magnetic loop of uniform cross-section; the mean path length gives the reluctance, Ampere's law gives the mmf and $H$, and the magnetic Ohm's law $\Phi = \mathcal{F}/\mathcal{R}$ closes the problem.

  1. Mean magnetic path length. The field follows the circular centre-line of the ring: $$\ell = 2\pi r_{av} = 2\pi(0.25) = 1.5708\ \text{m}.$$
  2. Reluctance of the circuit (a). With permeability $\mu = \mu_0\mu_r$, $$\mathcal{R} = \frac{\ell}{\mu_0\mu_r A} = \frac{1.5708}{(4\pi\times10^{-7})(1500)(3\times10^{-4})}.$$ Evaluating the denominator, $\mu_0\mu_r A = 5.655\times10^{-7}\ \text{Wb/A}\cdot\text{t}$, so $$\boxed{\mathcal{R} = 2.78\times10^{6}\ \text{A}\cdot\text{t/Wb}.}$$
  3. Magnetomotive force (b). The mmf is simply the ampere-turns of the coil: $$\mathcal{F} = N I = (600)(1.5) = 900\ \text{A}\cdot\text{t}.$$
  4. Magnetic field intensity (b). By Ampere's law around the mean path, $$H = \frac{\mathcal{F}}{\ell} = \frac{NI}{\ell} = \frac{900}{1.5708} = 573\ \text{A/m}.$$
  5. Flux (c). Using the magnetic Ohm's law, $$\Phi = \frac{\mathcal{F}}{\mathcal{R}} = \frac{900}{2.78\times10^{6}} = 3.24\times10^{-4}\ \text{Wb} = 0.324\ \text{mWb}.$$
  6. Flux density (c). Dividing the flux by the core area, $$B = \frac{\Phi}{A} = \frac{3.24\times10^{-4}}{3\times10^{-4}} = 1.08\ \text{T}.$$ As a cross-check, $B = \mu_0\mu_r H = (4\pi\times10^{-7})(1500)(573) = 1.08\ \text{T}$, which agrees.
Final results — Question 1
QuantitySymbolValue
Reluctance$\mathcal{R}$$2.78\times10^{6}$ A·t/Wb
Magnetomotive force$\mathcal{F}$900 A·t
Field intensity$H$573 A/m
Flux$\Phi$0.324 mWb
Flux density$B$1.08 T
← Paper overview