An ideal transformer is designed to convert 50 V into 250 V. It draws 200 W power from an AC source whose instantaneous voltage is given by \( v_i = 20 \sin(100\pi t) \, \text{V} \).
Find:
Given data:
1. RMS value of input voltage: The given instantaneous input voltage is of the form \( v_i = V_p \sin(\omega t) \), where \( V_p = 20 \, \text{V} \) is the peak voltage. The RMS value \( V_{\text{rms}} \) is related to the peak voltage \( V_p \) by:
\[ V_{\text{rms}} = \frac{V_p}{\sqrt{2}} = \frac{20}{\sqrt{2}} = 14.14 \, \text{V} \]
2. RMS value of input current: The power \( P \) supplied by the AC source is related to the RMS values of voltage and current by the formula:
\[ P = V_{\text{rms}} I_{\text{rms}} \cos \phi \]
For an ideal transformer, \( \cos \phi = 1 \), since the transformer ideally operates at unity power factor. Therefore:
\[ I_{\text{rms}} = \frac{P}{V_{\text{rms}}} = \frac{200}{14.14} \approx 14.14 \, \text{A} \]
Thus, the RMS value of input current is \( 14.14 \, \text{A} \).
For an ideal transformer, the ratio of the voltages is equal to the ratio of the number of turns in the primary and secondary coils:
\[ \frac{V_s}{V_p} = \frac{N_s}{N_p} \]
This means the output voltage is related to the input voltage by the ratio of turns. Since \( V_p = 50 \, \text{V} \) and \( V_s = 250 \, \text{V} \), the transformer steps up the voltage by a factor of 5. Hence, the instantaneous output voltage \( v_s \) is:
\[ v_s = 5 v_i = 5 \times 20 \sin(100\pi t) = 100 \sin(100\pi t) \, \text{V} \]
Thus, the expression for the instantaneous output voltage is \( v_s = 100 \sin(100\pi t) \, \text{V} \).
Using the relationship between the current and voltage in an ideal transformer:
\[ \frac{I_s}{I_p} = \frac{V_p}{V_s} \]
Since \( V_p = 50 \, \text{V} \) and \( V_s = 250 \, \text{V} \), the current in the secondary will be reduced by the same factor of 5. Thus, the instantaneous output current \( i_s \) is related to the input current \( i_p \) by:
\[ i_s = \frac{I_p}{5} \]
The input current \( i_p \) is related to the instantaneous input voltage by Ohm’s law:
\[ i_p = \frac{v_i}{R} = \frac{20 \sin(100\pi t)}{400} = 0.05 \sin(100\pi t) \, \text{A} \]
Thus, the instantaneous output current \( i_s \) is:
\[ i_s = \frac{0.05 \sin(100\pi t)}{5} = 0.01 \sin(100\pi t) \, \text{A} \]
Thus, the expression for the instantaneous output current is \( i_s = 0.01 \sin(100\pi t) \, \text{A} \).
Predict the direction of induced current in the situations described by the following Figs. 6.18(a) to (f ).
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