Answer
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Hint: In circuits with essentially capacitive loads, current leads to the voltage. Current must first move to the two plates of the capacitor, where a charge is collected. Only after charge stores at the plates of a capacitor is a voltage difference set.
Complete step-by-step solution:
Given: $V(t) = (80V) sin wt$
$I(t) = (1.6A) sin\left( wt + \dfrac{\pi}{4} \right)$
As we can see, current leads to voltage.
This circuit is capacitive.
The black box contains at least one resistor and capacitor.
$\lt P_{av} \gt = \dfrac{V_{m} I_{m}}{2}$
We have, $V_{m} = 80V$
$I_{m} = 1.6A$
Put all the given values,
$\lt P_{av} \gt = \dfrac{80 \times 1.6}{2} cos\dfrac{\pi}{4}$
$\implies \lt P_{av} \gt = 45.25 W$
When capacitors are combined across a direct current DC voltage, their plates charge to the voltage value crossed; the capacitor is equal to that of the externally connected voltage. The capacitor will operate this charge regularly, acting as a transient storage device as long as the implemented voltage is kept.
Note:The movement of electrons onto the plates of a capacitor is directly proportional to the rate of change of the voltage across those plates. Then, we can observe that capacitors in AC circuits like to move current when the voltage across its plates constantly changes concerning time, such as in AC signals, but it does not like to move current when the implemented voltage is of a constant value DC signals.
Complete step-by-step solution:
Given: $V(t) = (80V) sin wt$
$I(t) = (1.6A) sin\left( wt + \dfrac{\pi}{4} \right)$
As we can see, current leads to voltage.
This circuit is capacitive.
The black box contains at least one resistor and capacitor.
$\lt P_{av} \gt = \dfrac{V_{m} I_{m}}{2}$
We have, $V_{m} = 80V$
$I_{m} = 1.6A$
Put all the given values,
$\lt P_{av} \gt = \dfrac{80 \times 1.6}{2} cos\dfrac{\pi}{4}$
$\implies \lt P_{av} \gt = 45.25 W$
When capacitors are combined across a direct current DC voltage, their plates charge to the voltage value crossed; the capacitor is equal to that of the externally connected voltage. The capacitor will operate this charge regularly, acting as a transient storage device as long as the implemented voltage is kept.
Note:The movement of electrons onto the plates of a capacitor is directly proportional to the rate of change of the voltage across those plates. Then, we can observe that capacitors in AC circuits like to move current when the voltage across its plates constantly changes concerning time, such as in AC signals, but it does not like to move current when the implemented voltage is of a constant value DC signals.
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