The transformer, shown in fig. 9 , outputs power at 415 V , along a copper cable 50 m in length, to an electrical machine. The total resistance of the copper conductor ( 100 m there and back) is $0.0493 \Omega$ at an operating temperature of $60^{\circ} \mathrm{C}$. The machine takes a current of 200 A .

a) What is the total power that the transformer is supplying to the machine and cable?
b) What is (i) the power loss in the cable, and (ii) what percentage is this of the total power supplied?
c) Often the conductor size is chosen not on the basis of the steady current required, but on the short circuit current that might occur. If in our wiring, a short circuit occurred at the machine end of the cable, a current of 6000 A could be expected. Explain why this current is significantly less than that calculated from the 415 V supply and the $0.0493 \Omega$ resistance of the cable.
d) If the circuit breaker produces a delay of 0.4 s before it breaks the circuit, calculate the heat energy generated in this short time interval. Assume that the resistance of the wire does not change significantly as it heats up.
e) The heat energy required to raise the temperature of 1 kg of copper by $1^{\circ} \mathrm{C}$ is called the specific heat capacity of copper. It has the value is $385 \mathrm{~J} \mathrm{~kg}^{-1}{ }^{\circ} \mathrm{C}^{-1}$. We can use a simple formula,
$$\text { heat energy supplied = mass } \mathbf{x} \text { specific heat capacity } \mathbf{x} \text { temperature rise }$$
in order to determine the temperature rise of the copper cable, assuming no heat loss to the surroundings.
Calculate
(i) The mass of copper in the 100 m of cable, given that its
$$\begin{aligned} \text { cross sectional area } & =50 \mathrm{~mm}^{2} \\ \text { density of copper } & =8960 \mathrm{~kg} / \mathrm{m}^{3} \end{aligned}$$
(ii) Calculate the final temperature of the cable after 0.4s, if its initial temperature is $60^{\circ} \mathrm{C}$.
Show worked solution
The transformer supplies power at 415 V with a current of 200 A. The total power is:
$$P_{total} = VI = 415 \times 200 = 83,000 \text{ W} = 83 \text{ kW}$$
b) Power loss in cable (i) Power loss:The cable has a resistance of $R = 0.0493$ $\Omega$. Using $P = I^2R$:
$$P_{loss} = I^2R = (200)^2 \times 0.0493$$
$$P_{loss} = 40,000 \times 0.0493 = 1,972 \text{ W} \approx 1.9 \text{ kW}$$
(ii) Percentage of total power:$$\text{Percentage} = \frac{P_{loss}}{P_{total}} \times 100\%$$
$$\text{Percentage} = \frac{1,972}{83,000} \times 100\%$$
$$\text{Percentage} = 0.0238\% \approx 2.3 \times 10^{-3} \%$$
c) Why short-circuit current is less than calculatedThe theoretical short-circuit current from the supply voltage and cable resistance would be: $$I_{theoretical} = \frac{V}{R} = \frac{415}{0.0493} = 8,418 \text{ A}$$
However, the actual short-circuit current is only 6000 A. The difference is due to the internal resistance of the transformer's secondary winding.
When calculating short-circuit current, we must include both: 1. The cable resistance: $0.0493$ $\Omega$ 2. The transformer secondary winding resistance: $R_{transformer}$
The total resistance is: $$R_{total} = R_{cable} + R_{transformer}$$
$$R_{total} = \frac{415}{6000} = 0.0692 \text{ }\Omega$$
Therefore: $R_{transformer} = 0.0692 - 0.0493 = 0.0199$ $\Omega$
d) Heat energy generated during short circuitDuring the 0.4 second delay before the circuit breaker activates:
$$E = VIt = 415 \times 6000 \times 0.4$$
$$E = 996,000 \text{ J} = 996 \text{ kJ}$$
e) Temperature rise of copper cable (i) Mass of copper in 100 m of cable:Given:
- Cross-sectional area: $A = 50$ mm$^2$ $= 50 \times 10^{-6}$ m$^2$
- Length: $L = 100$ m (50 m there and 50 m back)
- Density of copper: $\rho = 8960$ kg/m$^3$
$$\text{Volume} = A \times L = 50 \times 10^{-6} \times 100 = 5 \times 10^{-3} \text{ m}^3$$
$$\text{Mass} = \rho \times \text{Volume} = 8960 \times 5 \times 10^{-3} = 44.8 \text{ kg}$$
(ii) Final temperature after 0.4 s:Using: $Q = mc\Delta T$
Where:
- $Q = 996,000$ J (heat energy)
- $m = 44.8$ kg (mass of copper)
- $c = 385$ J/(kg$\cdot^\circ$C) (specific heat capacity)
- $\Delta T$ = temperature rise
$$996,000 = 44.8 \times 385 \times \Delta T$$
$$\Delta T = \frac{996,000}{44.8 \times 385} = \frac{996,000}{17,248} = 57.7^\circ \text{C} \approx 58^\circ \text{C}$$
Final temperature: $$T_{final} = T_{initial} + \Delta T = 60^\circ \text{C} + 58^\circ \text{C} = 118^\circ \text{C}$$
Note: This rapid temperature rise demonstrates why circuit breakers must act quickly to prevent fire hazards!


























