22-Elec-A6 Power Systems and Machines · Undated paper
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
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 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.
| 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.
| Quantity | Symbol | Value |
|---|---|---|
| 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 |