Solution Electrical Numerical 11
Numerical 11: A
moving coil ammeter, a thermal ammeter and a rectifier are connected in
series with a resistor across a 110 V sinusoidal a.c. supply. The
circuit has a resistance of 50Ω to current in one direction and, due to
the rectifier, an infinite resistance to current in the reverse
direction. Calculate:
(i) The readings on the ammeters; (ii) The form and peak factors of the
current wave.
Solution:
(i) Max value of voltage: $\displaystyle \displaystyle \mathrm{V_m\ =\
\frac{V}{0.707}\ =\ \frac{110}{0.707}\ =\ 155.5\, V }$
Max Value of current: $\displaystyle \displaystyle \mathrm{I_m\ =\ \frac{V_m}{R}\ =\ \frac{115.5}{50}\ =\ 3.11\, A }$
During
the +ve half cycle the current is proportional to the voltage and is
sinusoidal (see figure). Thus average value of current over the +ve half
cycle.
.
$\displaystyle \displaystyle \mathrm{I_{av}\ =\ 0.637\times I_m =\ 0.637\times 3.11 =\ 1.98\ A}$
During
-ve half cycle, the current is zero. But because of inertia of the
moving system the moving coil ammeter reads the average value of the
current over the whole cycle.
Therefore reading on the Moving coil ammeter: $\displaystyle \displaystyle \mathrm{\frac{1.98}{2} =\ 0.99\ A}$
The variation of the heating effect in the thermal ammeter is shown in the figure, the max power being $\displaystyle \mathrm{I_{m}^{2}R}$ where R is the resistance of the instrument.
The
average heating effect over the +ve half cycle is $\displaystyle
\mathrm{\frac{1}{2}I_{m}^{2}R}$ and since no heat is generated during
the 2nd half cycle, it follows that the average heating effect over a
complete cycle is $\displaystyle \mathrm{\frac{1}{4}I_{m}^{2}R}$
If I is the direct current which produce the same heating effect then,
$\displaystyle \mathrm{I^2R\ =\ \frac{1}{4}I_{m}^{2}R}$
$\displaystyle \mathrm{I\ =\ \frac{1}{2}I_{m}\ =\ \frac{3.11}{2} =\ 1.555\ A }$
i.e Reading on thermal ammeter =1.555 A
[ don't use $\displaystyle \mathrm{I\ =\ \frac{0.707\times 3.11}{2} =\ 1.1\ A }$ ]
(ii) Foam factor: $\displaystyle \mathrm{K_f\ =\ \frac{I}{I_{av}} =\ \frac{1.555}{0.99} =\ 1.57 }$
Peak factor: $\displaystyle \mathrm{K_P\ =\ \frac{I_m}{I} =\ \frac{3.11}{1.555} =\ 2.0 }$
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