Fig. 10.1 shows a simple laminated iron-cored transformer consisting of a primary coil of 25000 turns and a secondary coil of 625 turns. The output potential difference (p.d.) VOUT is applied to a load resistor of resistance 640Ω. [Figure 10.1] [Figure 10.2]
- (a)(i)State the function of the iron core.[1]
- (a)(ii)Explain why the iron core is laminated.[2]
- (b)(i)The input p.d. VIN is a sinusoidal alternating voltage of peak value 12kV and period 40ms. Calculate the maximum value of VOUT.[1]
- (b)(ii)Calculate the root-mean-square (r.m.s.) current in the load resistor.[1]
- (b)(iii)On Fig. 10.2, sketch the variation with time t of the power P dissipated in the load resistor for time t = 0 to t = 40 ms. Assume that P = 0 when t = 0.[3]
- (c)Explain, with reference to Fig.10.2, why the mean power in the load resistor is 70W.[2]
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Mark scheme
Marking points from the official mark scheme (Oct/Nov 2021). The mark or mark type is shown in brackets.
- to increase the magnetic flux linkage (between the coils)
- to reduce energy losses
- by reducing induced currents
- maximum VOUT = 12 000 × (625/25000)
- = 300 V
- r.m.s. current = 300 / (640 × √2)
- = 0.33 A
- sketch: sinusoidal shape in positive half of the graph, sitting with ‘minima' resting on the time-axis (at P = 0)
- each 'cycle' shown repeating every 20 ms
- maximum P shown as 140 W
- power curve is symmetrical about the midpoint (on the power axis)
- mean power is half the peak power
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