Concept:
• An ideal transformer is assumed to be $100\%$ efficient, meaning absolutely zero power is lost during the transfer.
• Input electrical power perfectly equals output electrical power ($P_{in} = P_{out}$).
• Electrical power for AC circuits (assuming unity power factor for simple transformer problems) is $P = V \cdot I$.
• The voltage elegantly scales strictly according to the turns ratio equation: $\frac{V_s}{V_p} = \frac{N_s}{N_p}$.
Step 1: Identify the explicitly given parameters
Number of turns heavily wound in the primary coil: $N_p = 100$.
Number of turns heavily wound in the secondary coil: $N_s = 5000$.
The total input power rigorously supplied to the primary: $P = 3.3 \text{ kW} = 3300 \text{ W}$.
The applied primary voltage: $V_p = 220 \text{ V}$.
Step 2: Calculate the primary current (I)
The electrical power fundamentally delivered to the primary coil is completely determined by the product of primary voltage and primary current.
\[ P = V_p \cdot I_p \]
To find the primary current $I_p$, we simply rearrange the formula:
\[ I_p = \frac{P}{V_p} \]
Substitute the known values heavily into the arranged equation:
\[ I_p = \frac{3300 \text{ W}}{220 \text{ V}} \]
Simplify the fraction carefully by removing a zero:
\[ I_p = \frac{330}{22} \]
Divide thoroughly to get the exact value:
\[ I_p = 15 \text{ A} \]
The current powerfully drawn by the primary coil is therefore precisely $15 \text{ A}$.
Step 3: Calculate the output voltage (II)
To precisely find the output (secondary) voltage, we must employ the fundamental transformer turns ratio formula derived earlier.
\[ \frac{V_s}{V_p} = \frac{N_s}{N_p} \]
We can dynamically rearrange this to solve specifically for the secondary voltage $V_s$:
\[ V_s = V_p \times \left( \frac{N_s}{N_p} \right) \]
Insert all the designated given values directly into this relation:
\[ V_s = 220 \times \left( \frac{5000}{100} \right) \]
First, neatly resolve the bracketed turns ratio, which signifies a massive step-up factor:
\[ \frac{5000}{100} = 50 \]
Now, multiply this substantial factor by the primary voltage:
\[ V_s = 220 \times 50 \]
\[ V_s = 11000 \text{ V} \]
This enormous output can also be written efficiently as $11 \text{ kV}$.
The final output voltage securely provided by the secondary coil is $11000 \text{ V}$.