Show that the power dissipated in a resistor connected to an AC power source with frequency \(\omega\) oscillates with frequency \(2 \omega\).

Short Answer

Expert verified
Answer: The frequency of power dissipation in a resistor connected to an AC power source with frequency ω is 2ω.

Step by step solution

01

1. Voltage across the resistor

The voltage across the resistor connected to an AC power source can be represented as: \(v(t) = V_m \cos(\omega t)\) where \(V_m\) is the maximum voltage and \(\omega\) is the angular frequency of the source.
02

2. Current through the resistor

According to Ohm's Law, the current through the resistor can be found by dividing the voltage across the resistor by its resistance: \(i(t) = \frac{v(t)}{R} = \frac{V_m \cos(\omega t)}{R}\) where \(R\) is the resistance of the resistor.
03

3. Power dissipated in the resistor

The power dissipated in the resistor can be found using the formula: \(P(t) = v(t) \cdot i(t) = \frac{V^2_m}{R}\cos^2(\omega t)\)
04

4. Expressing power in terms of trigonometric identity

We can simplify the expression further by using the double-angle trigonometric identity: \(\cos^2(\omega t) = \frac{1 + \cos(2\omega t)}{2}\) So, substituting the trigonometric identity into the power equation, we get: \(P(t) = \frac{V^2_m}{R}\left (\frac{1 + \cos(2\omega t)}{2}\right)\)
05

5. Frequency of power dissipation

Now, we can see that the power dissipation function has a term \(\cos(2\omega t)\), which means that the power dissipated in the resistor oscillates with a frequency of \(2\omega\). So, we have shown that the power dissipated in a resistor connected to an AC power source with frequency \(\omega\) oscillates with frequency \(2\omega\).

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