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What is the rms current through a resist...

What is the rms current through a resistor of `50 Omega` when an alternating voltage given by `V 140 sin(314)t` is connected to it?

A

`1.5A`

B

`1.98A`

C

`2.5A`

D

`2.98A`

Text Solution

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The correct Answer is:
To find the RMS current through a resistor of 50 ohms when connected to an alternating voltage given by \( V = 140 \sin(314t) \), we can follow these steps: ### Step 1: Identify the RMS Voltage The given voltage is in the form \( V(t) = V_m \sin(\omega t) \), where \( V_m \) is the maximum voltage (amplitude) and \( \omega \) is the angular frequency. Here, \( V_m = 140 \) volts. The RMS (Root Mean Square) voltage \( V_{rms} \) for a sinusoidal voltage is given by the formula: \[ V_{rms} = \frac{V_m}{\sqrt{2}} \] ### Step 2: Calculate the RMS Voltage Substituting the value of \( V_m \): \[ V_{rms} = \frac{140}{\sqrt{2}} = \frac{140}{1.414} \approx 98.99 \text{ volts} \] ### Step 3: Use Ohm's Law to Find RMS Current Ohm's Law states that the current \( I \) through a resistor is given by: \[ I = \frac{V}{R} \] where \( V \) is the voltage across the resistor and \( R \) is the resistance. ### Step 4: Substitute Values to Find RMS Current Now substituting the values we have: \[ I_{rms} = \frac{V_{rms}}{R} = \frac{98.99}{50} \] Calculating this gives: \[ I_{rms} \approx 1.9798 \text{ A} \] ### Step 5: Round the Answer Rounding to two decimal places, we get: \[ I_{rms} \approx 1.98 \text{ A} \] Thus, the RMS current through the resistor is approximately **1.98 A**. ---

To find the RMS current through a resistor of 50 ohms when connected to an alternating voltage given by \( V = 140 \sin(314t) \), we can follow these steps: ### Step 1: Identify the RMS Voltage The given voltage is in the form \( V(t) = V_m \sin(\omega t) \), where \( V_m \) is the maximum voltage (amplitude) and \( \omega \) is the angular frequency. Here, \( V_m = 140 \) volts. The RMS (Root Mean Square) voltage \( V_{rms} \) for a sinusoidal voltage is given by the formula: \[ V_{rms} = \frac{V_m}{\sqrt{2}} ...
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