Peak And R.M.S Value Of An Alternating Current / Voltage

What is an Alternating current?

Alternating current can be defined as the current whose magnitude may change with time and also reverses the direction periodically.

The general equation is given by,

\(I\) = \(I_o ~sin~ ωt\)

\(I\) = \(I_o ~cos~ ωt\)

Where, \(I_o\) is termed as peak value of an alternating current.

Alternating Current

Considering the above equation the current changes at any instantaneous time, if the current is passed through the electric circuit and it can be assumed to remain constant for any small time dt. As current is passed for short time a small amount of charge is flown through the circuit in time dt and it is represented as:

If the current ‘\(I\)’ is indicated as a sine function then,

\(I\) = \(I_o ~sin~ ωt\)

\(dq\) = \(I ~dt\)

\(dq\) = \(I_o~ sin~ ωt~dt\)

At half the period of an alternating current, the amount of charge passed through the circuit at time

\(\frac{T}{2}\) is given by:

\(q\) = \(\int\limits_{0}^{\frac{T}{2}} I_0 sin~ωt~dt\)

\(q\) = \(I_0 \int\limits_{0}^{\frac{T}{2}} sin~ωt~dt\)

\(q\) = \(I_0 [\frac{-cos ~ωt}{ω}]_{0}^{\frac{T}{2}}\)

\(q\) = \(\frac{-I_0}{ω} [cos~ωt]_{0}^{\frac{T}{2}}\)

\(q\) =  \( \frac{-I_0 ~T}{2\pi} [cos~\pi ~-~ cos~0]\)

\(q\) =  \(\frac{-I_0~T}{2\pi}[-1 -1]\)

\(q\) = \(\frac{I_0~T}{\pi}\)      ……….equation (1)

The mean value of the alternating current is given by,

\(q\) = \( I_m. ~\frac{T}{2}\)      ……..equation (2)

On equating equation (1) and equation (2), we get:

\(I_m.~\frac{T}{2} \) = \( \frac{I_0~T}{\pi}\)

\(I_m\) = \(\frac{2I_0}{\pi}\) = \(0.636~ I_0\)

Do you know what will happen to the mean square value of an alternating current when it completes its full cycle?

The mean value of alternating current for completing the full cycle will be zero.

RMS Value of Alternating Current

RMS stands for root mean square of instantaneous current values. The RMS value of alternating current is given by direct current which flows through a resistance. The RMS value of AC is greater than the average value. The RMS value of sine current wave can be determined by the area covered in half-cycle. This is applicable to all the waves which inclues sinusoidal, non-sinusoidal, symmetrical, and asymmetrical. It is denoted by Irms or Iv.

RMS Value of AC Formula

Following is the formula of RMS value of AC:

\(I_{r.m.s}\) = \(\frac{I_0}{√2} \)\(0.707 ~{I_0}\)

RMS Value of AC Derivation

\(I\) = \(I_o~ sin~ ωt\)

\(dH\) = \(I^2~ R~dt\)

\(dH\) = \((I_0~sin~ωt)^2~R~dt\)

\(dH\) = \(I_0^2~R~sin^2~ωt~dt\)

The heat produced in a time \(\frac{T}{2}\) is given by:

\(H\) = \(\int\limits_{0}^{\frac{T}{2}}~{I_0}^2~R~sin^2~ωt~dt\)

\(H\) = \({I_0}^2~R~\int\limits_{0}^{\frac{T}{2}} sin^2~ωt~dt\)

\(H\) = \(\frac{{I_0}^2~R}{2}[\frac{T}{2}~-~0]\) = \(\frac{{I_0}^2~R}{2}.\frac{T}{2}\)         ……equation (3)

The rms value of AC is represented as:

\(H\) = \( {I_{r.m.s}}^2~R.~\frac{T}{2}\)        ………equation (4)

By equating equation (3) and equation (4), we get:

\({I_{r.m.s}^2}~R.~\frac{T}{2}\) = \(\frac{{I_0}^2 ~R}{2}. \frac{T}{2}\)

\({I_{r.m.s}^2}\) = \(\frac{{I_0}^2}{2}\)

\(I_{r.m.s}\) = \(\frac{I_0}{√2} \)= \(0.707 ~{I_0}\)

These values are measured by Ammeter and Voltmeter that are used in the circuit.

 

Leave a Comment

Your email address will not be published. Required fields are marked *