Blog #21 - Sinusoidal Waves & RMS Values

This video is part of my series on alternating current. In this video, we are going to define RMS values. You will find this topic along with others in my course entitled Basic Fundamentals of AC Circuit Analysis. You can access this and my other courses on my stand store at this web address.

As we communicate the value of voltage and current with others in the industry of electrical power, we have to ask ourselves how useful are using any of the terms and is there some way of measuring the values that is the most useful way. That question was asked and answered a long time ago and the answer was the RMS values.

Before just jumping to the definition of RMS, which by the way is mathematically related proportionally to amplitude peak, peak to peak, average and mean average values, let's go through some logical steps to get there. Starting with two simple circuits, one DC, one AC. That is, each with the same load but one driven by DC source and the other driven by an AC source.

When we close the switch on the DC circuit, the bulb will light with an intensity that is dependent on the resistance, RL, of the light and the DC current.

Now let's close the switch and adjust the AC current to the light bulb with the same Intensity. That is to say both loads, both lights consume the same average power. So we now ask ourselves what is that AC current?

We can come to the conclusion that if the two bulbs light to the same brightness, that is they draw the same amount of power and it is reasonable to consider the current IAC to be in some ways equivalent to the current IDC. So what is that value of AC?

It would be useful if there was some meaningful way to calculate it. So let's go there. If an AC supply is connected to a component of resistance, say R, the instantaneous power dissipated is given by the power equation I squared R. If we plot I2, the instantaneous current, which itself is a sine wave, it is always positive because plus I times plus I is positive and negative I times negative I is positive. It does go to zero but never negative.

Remember that the instantaneous power dissipated is given by the equation power equals I2R. The peak or maximum value of I2 is shown here and labeled I2 max. The mean or average value of I2 is I2 max divided by two.

So the average value of power is, I will call it PAV is equal to I2max over 2RL. We just saw from the previous slide that the average power consumed in the circuit is given by this equation which is equal to the maximum value of the current squared over two times the resistor.

Let's define a current that when used to calculate power gives us the average power. In other words, when that current, let's call it Idefined for now, is squared and multiplied by RL gives us the average power.

But the defined or I2defined is also equal to I2max over two. Therefore, the square root of the mean current equals that defined current.

So we just discovered that what the value of Idefined is equal to I max divided by root two…and we call this current IRMS…or root mean square and it is 0.707 the value of the maximum current.

This is another more useful way to describe AC quantities, voltage and current. And of course it can be converted directly to amplitude peak or peak to peak or average just by multiplying by a scaling factor. However, we use RMS values for current and voltage.

We can directly calculate the average power from these root mean square quantities.

This video is part of my electrical technical information series. In this series, I will be covering essential topics to help you understand electrical systems.Be sure and stay tuned as I will also, from time to time, be reviewing electrical products that in my opinion are worthy of paying attention to.

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