RMS VALUE OF NON SINUSOIDAL WAVE — Transcript
Full transcript
- 0:01Good day everyone. So welcome to our to
- 0:05the continuation of our
- 0:08discussion on the topic
- 0:11nonosoidal waves. So I really now
- 0:15excited to guide you through the topic
- 0:19that plays a vital role in modern
- 0:23electrical
- 0:24engineering. So this is the RMS or the
- 0:27effective value of the sinusoidal wave
- 0:31form. So in this
- 0:33presentation we go beyond the typical
- 0:35side wave and explore how to deal with
- 0:38real world signals which are of
- 0:41irregular and complex in shape. So let's
- 0:46begin.
- 0:52So in electrical engineering the
- 0:55effective value or the RMS or root
- 0:58square is used to express an alternating
- 1:03quantity in terms of its equivalent DC
- 1:08value particularly in how it delivers
- 1:11power to a resistive load while senosal
- 1:17wave form are often used in theory and
- 1:20textbooks. Most practical signals like
- 1:23those found in power electronics and
- 1:26digital systems are nonsenosidal.
- 1:30So for example we have this square waves
- 1:34triangular
- 1:36waves and complex distorted signals.
- 1:40That is why understanding how to compute
- 1:45RMS values for such wave forms is both a
- 1:48theoretical necessity and a practical
- 1:55skill. So let's define it formally. The
- 1:59root means square value of a periodic
- 2:01wave form is equivalent to the square
- 2:04root of the
- 2:06average of the squares of the
- 2:08instantaneous values over one cycle. So
- 2:13we will just we will use this formula
- 2:18no. So why is the RMS
- 2:24value? This is because it reflects the
- 2:28true power capability of an AC source.
- 2:33In resistive
- 2:34circuits, it determines how much thermal
- 2:38energy will be generated.
- 2:40Whether we analying power supplies,
- 2:44motors and communication signals, RMS
- 2:48provides a consistent and comparable
- 2:52measure of
- 2:54energy. In essence, it gives us a fair
- 2:58comparison between AC and
- 3:02DC power.
- 3:09So now let's explore the core of our
- 3:12topic. How to calculate RMS for
- 3:17nonsenosoidal wave form. Unlike pure
- 3:20sinusoids, nonsinosoidal signals may
- 3:23contain multiple harmonics or follow
- 3:26shapes like square or triangular
- 3:30patterns. So for example we have the
- 3:33square wave. So to compute for the
- 3:35amplitude or I mean for the RMS value of
- 3:40this wave. So we have here the piece
- 3:44wise function. So for
- 3:47example you have this square wave no
- 3:51from 0 up to time t for one full cycle
- 3:56or one period. So labeled as T sub O. So
- 4:01half of it will be equivalent to t / 2
- 4:06and the other half is t / 2. So for the
- 4:10first function from
- 4:130 to t / 2 you have this a no equation a
- 4:20from 0 to t / 2 and from t / 2 to t so
- 4:27you have this -
- 4:30a just substitute this to our
- 4:34formula okay so for the full cycle for
- 4:37one cycle of the wave
- 4:39have this the positive cycle plus the
- 4:42negative RMS of the negative cycle. So
- 4:46after manipulating the
- 4:48integral so come up with the value of
- 4:51the RMS of a square wave equivalent to
- 4:56its
- 4:58amplitude. Next.
- 5:02So for a triangular wave having a pick
- 5:04value of a so RMS value is equivalent to
- 5:08the amplitude divided by s root of 3. So
- 5:14the derivation of this formula will be
- 5:17left as your
- 5:20exercise. And also for a soot wave for a
- 5:24pick value of a
- 5:26again so we have a value of a divided by
- 5:30s root of 3. So take note of this
- 5:35quantities or
- 5:40equations. So for a general complex wave
- 5:43so the instantaneous current as a for
- 5:45example this instantaneous current as a
- 5:48function of time. So this is composed of
- 5:52several harmonics no so they have
- 5:55fundamental second third up to and
- 5:59harmonic so a sub0er here represents the
- 6:02dc component so im1 im2 im3 imn are the
- 6:09maximum values of each harmonic and
- 6:14alpha 2 alpha 3 are the face angl
- 6:20and omega is our angular frequency and t
- 6:24represents the time.
- 6:28So let's solve for or let's find a
- 6:32formula in solving for the RMS value of
- 6:37this complex wave.
- 6:41So we will just use the formula for
- 6:46solving the RMS value. So we just
- 6:49substitute the instantaneous value or
- 6:52the instantaneous
- 6:53equation. So you have this quantity
- 6:57square dt from 0 to t for one period or
- 7:03for one whole cycle.
- 7:05So after manipulating this integral so
- 7:09come up with this effective value or RMS
- 7:12value equivalent
- 7:13to square root of the DC component squ
- 7:16plus the summation of the individual
- 7:19maximum value on each harmonic and
- 7:23squares so divided by
- 7:262 and also we can express that equation
- 7:30in terms of RMS value of each harmony.
- 7:35Okay.
- 7:38So uh take note that RMS is equivalent
- 7:41to the maximum value divided by SO 2 for
- 7:45aign wave. Ha? This is just applicable
- 7:47for a sign
- 7:49wave. So I over s root of 2. So
- 7:55substituting this value to the equation
- 7:58previous equation. So we arrive on
- 8:02this uh formula for RMS value in terms
- 8:06of the RMS value of each
- 8:10harmonic. Okay. So we can also use this
- 8:13formula if you are solving for harmonic
- 8:16of each uh RMS value of harmonic so you
- 8:19can use this formula.
- 8:26And also we can also solve for the power
- 8:30no power due to
- 8:32anosidal voltage so we have here the
- 8:35general expression for the average
- 8:37power in a circuit with time varying
- 8:41voltage and current given as this
- 8:43equation.
- 8:45So I already introduced this equation to
- 8:48you in our previous
- 8:50discussions. 1 / t integral of e of t or
- 8:55the instantaneous value of voltage times
- 8:57instantaneous value of current dt over 1
- 9:01period from 0 to t.
- 9:05So for example if you have
- 9:08this nonsusidal voltage oranous voltage
- 9:12equivalent is em sub 1 sin omega t +
- 9:16alpha 1 + em sub 2 sin 2 omeg t so and
- 9:19so forth and for
- 9:22current im sub 1 sin omega t + alpha 1
- 9:26prime 1. So we just substitute
- 9:30this uh equations to our formula for
- 9:36power then integrate it from 0 to t for
- 9:40one period. So after integrating the
- 9:44equation or the
- 9:47integral so we come up with this formula
- 9:51for power. So is this is this is just a
- 9:55summation of uh its maximum product of
- 10:00maximum value of each harmony divided by
- 10:042 and cosine of the difference of the
- 10:07two phase
- 10:09angles. So em sub 1 and im sub one
- 10:12corresponds to the fundamental harmonic
- 10:14and you will also use the uh face angle
- 10:18of its harmonic of fundamental harmonic.
- 10:22So for voltage you have alpha 1 and for
- 10:25current alpha prime
- 10:281. Every everything will just
- 10:32follow. So take note of the
- 10:39formula. So to to better understand our
- 10:43formula. So let's apply it to our
- 10:46example. So find the power represented
- 10:49by the following
- 10:52given. So instantaneous voltage
- 10:54equivalent to 100 sin omega t + 30 - 50
- 11:00sin 3 om t + 60. So 25 + 5 sin 5 omeg t
- 11:08and for current 20 sin omega t - 30 + 15
- 11:13sin 3 om t + 30 + 10 cos 5 omeg t - 60
- 11:19amp. So we have now this
- 11:22two uh instantaneous values of voltage
- 11:26and current. So for the voltage it is
- 11:30expressed in terms of a sign function
- 11:33and for current
- 11:36so expressed in sign and the fifth
- 11:40harmonic is expressed in terms of
- 11:44cosine. So before solving or before
- 11:47applying the formula see to it that the
- 11:50quantities
- 11:51are consistent. So meaning if in the
- 11:55fifth
- 11:56harmonic you are using sign of course in
- 11:59the fifth harmonic of the instantaneous
- 12:03current it should also be sign so we
- 12:08convert this function or this equation
- 12:10in terms of
- 12:13sin so recall the formula that
- 12:19cosθ is equivalent
- 12:22to sin
- 12:26ofθa +
- 12:3190°. Okay. So
- 12:36substitute sin
- 12:38of 5 omeg
- 12:43t -
- 12:4660 + 90.
- 12:51So this quantity 10 cos 5 omeg t- 60° is
- 12:55equivalent to
- 12:5810 sin
- 13:02of
- 13:045 omega
- 13:10t
- 13:13plus 30.
- 13:15Okay. So this this is the equivalent sin
- 13:19of this cosine quantity. So we can now
- 13:23use the formula.
- 13:27Okay. So, so for for the fundamental
- 13:30harmonic so the maximum value for
- 13:33voltage is 100 times the maximum value
- 13:36for current 20/ 2 cos of the face angle
- 13:41of the voltage which is 30
- 13:45minus cos uh minus the face angle of the
- 13:48current which is nega 30.
- 13:53Next for in the third
- 13:56harmonic so will have
- 13:59-50
- 14:0115/ 2 cos of the face angle of the
- 14:06voltage the third harmonic which is
- 14:0960 min the face angle of
- 14:15the current the harmonic 30 and in theth
- 14:20harmonic
- 14:22So we have this maximum value of
- 14:2525
- 14:2710/ 2 cos of the face angle of the fifth
- 14:32harmonic is zer so 0 min the face angle
- 14:38of the third harmonic which
- 14:40is I mean in the fth harmonic which is
- 14:4430
- 14:46so after substituting the vales
- 14:50No. So you can now solve for by
- 14:54using your calculators. You can solve
- 14:57for current or the power I
- 15:00mean.
- 15:01Okay. So for this quantity you have this
- 15:06500 watts. And for the next quantity for
- 15:11the third harmonic you have - 324.75 75
- 15:15and for the fifth harmonic you will have
- 15:18108.25
- 15:2025. So summing up all of this will
- 15:25result to the power which is equivalent
- 15:29to
- 15:33283.5. Okay. So let's proceed to the
- 15:40next. So we have here another example.
- 15:44So find the power delivered by the
- 15:48following instantaneous values of
- 15:51voltage and current.
- 15:54So you have here for the voltage you
- 15:56have a value 100 sin omega t + 50 sin 5
- 16:01omeg t- 80- 40 cos and for the current
- 16:07we have 30 sin of omeg t +
- 16:1160 sin of 5 omeg t - 50 and sin 7 10 sin
- 16:177 omeg t + 60 so as you can observe that
- 16:23the seventh harmonic for the voltage
- 16:25source is expressed in terms of cosine.
- 16:30So we convert this into sin. Okay. So s
- 16:36function so step one we have here
- 16:39convert all to sign function. So the -
- 16:4240 cos 7 om t + 30 is equivalent to in
- 16:47terms of s this is equivalent to
- 16:50-47 omeg t +
- 16:5520°. So solving for the
- 16:58power same as what we did on the
- 17:00previous
- 17:02example solve for the
- 17:05individual power on
- 17:07its harmonic. So in the fundamental
- 17:11harmonic you have here 100
- 17:1530/ 2 cosine of so your face angle for
- 17:20the fundamental harmonic of your voltage
- 17:23is
- 17:24zero and for your current is 60 so 0-
- 17:2960 so using using your
- 17:33calculator so you will come up of this
- 17:36on this value of 750 50 wat and next in
- 17:41the fifth harmonic you have
- 17:44433 and in the 7th harmonic you
- 17:47have 100 so take the sum of this three
- 17:52powers no so you come up with this value
- 17:58of value of power which is equivalent
- 18:08So ah
- 18:13okay this value of
- 18:22sorry
- 18:27okay so volt ampires or your
- 18:34uh apparent power and power factor for
- 18:38nonosidal waves. So the volt amper
- 18:41apparent for the apparent power. So volt
- 18:44amper so this is determined by the
- 18:46product of the effective voltage and the
- 18:48effective current.
- 18:50So you are already familiar with
- 18:54it that S or the apparent power is
- 18:57equivalent
- 18:59to the voltage times the current SBI. So
- 19:05this is in
- 19:08terms for the volt
- 19:10amper we just use this formula. So take
- 19:15the RMS value of the voltage no and also
- 19:19take the RMS value of the
- 19:21current and multiply
- 19:25it. So for
- 19:27example so in our previous
- 19:29example you have here the
- 19:33the RMS value for
- 19:36voltage and RMS value for current. So
- 19:39just take the RMS value of each
- 19:41quantity.
- 19:43Sige. So, so you have here the value
- 19:49for it's a parent power equivalent to
- 19:5510001
- 19:56vol. So just take
- 19:59the uh RMS value of the voltage and the
- 20:03RMS value of the current and multiply
- 20:07them will have the amp the apparent
- 20:12power.
- 20:14Next. So for the power factor so power
- 20:18factor this is the ratio
- 20:23between ratio between the real power and
- 20:26the apparent power. So this is a measure
- 20:30of how much real power has been consumed
- 20:34for the given apparent power. Okay. So
- 20:39you just substitute the formula. So this
- 20:41is the formula for the real power p no
- 20:46real power p
- 20:49and the denominator is the apparent
- 20:58power so this is p or
- 21:03div va
- 21:06or vol ampes
- 21:12So for example in our previous example
- 21:15in example 6 so we compute we computed
- 21:19this equivalent wats no power and in our
- 21:23prev example 7 so we computed
- 21:27this volt amp the apparent so just
- 21:31divide
- 21:32p
- 21:34va come up with this with this this
- 21:38value
- 21:39of our
- 21:43factor. So na siya no ratio between the
- 21:49real power and the apparent
- 21:56power. Okay. So let's now come to
- 21:59circuit analysis when waves are
- 22:02nonsenosoidal.
- 22:04So we just walk through on this example
- 22:07to better understand how we're going to
- 22:09analyze a
- 22:11circuit when our source source voltage
- 22:16and current are expressed in
- 22:21nonosoidal. So for
- 22:23example given the circuit with the
- 22:26parameter shown
- 22:30so these are the parameters of our
- 22:33circuit. So a series
- 22:35circuit no so when omega or the angular
- 22:38frequency is 377 radians per second and
- 22:43the voltage source is
- 22:45141.4 sin omega t + 70.7 sin 3 om t +
- 22:5130° - 28.28 28 sin 5 omeg t-
- 22:5620° volt is impressed.
- 23:00find the current I so the reading if you
- 23:04have if you connect here an
- 23:08ameter that ameter would read and also
- 23:11find the total power dissipated and the
- 23:15effective value of voltage drop across
- 23:18the inductance and also find the
- 23:21equation for the current wave so to
- 23:27solve this problem no uh we will
- 23:30consider the current on each fonda on
- 23:36each on each harmonic. So for let's
- 23:39first analyze using the fundamental
- 23:41harmonic and second let's analyze the
- 23:45current or the voltage drop in the third
- 23:49harmonic and also in the fifth harmonic.
- 23:54So first let's do the analysis in the
- 23:58fundamental harmonic. So we have the
- 24:00given. So you have R equ to 6 ohms L
- 24:050.05 Henry and 98.8
- 24:09microfarad. Then the source voltage is
- 24:13given. So what we are going to solve is
- 24:17the current
- 24:18I the total power dissipated effective
- 24:21value for voltage drop across the
- 24:24inductor and in equation of the current
- 24:28wave. So take note that the ameter would
- 24:30only read
- 24:32RMS value ha the effective
- 24:35value. That's what our ameter would
- 24:39read. So first let's analyze the circuit
- 24:43in the
- 24:45fundamental harmonic. Okay. So
- 24:49fundamental
- 24:50harmonic. So you have your voltage
- 24:52number one equivalent
- 24:55to so in the fundamental harmonic. So
- 24:58you have this value
- 25:00of your voltage maximum
- 25:04141.4. So ah let's solve for its RMS
- 25:09value. So we will divide it by root of 2
- 25:14since this is expressed in sign. So
- 25:16141.4
- 25:174
- 25:192 100
- 25:23volt inductance in the fundamental
- 25:25harmonic so we will use the omega
- 25:28equivalent to
- 25:32377 this is because in the fundamental
- 25:36harmonic you have your angular frequency
- 25:38as
- 25:41omega okay so 377 times the inductance
- 25:45you have this
- 25:4718.85 ohms and for your capacitance or
- 25:51capacitive reactance again use
- 25:55the
- 25:57value of omega to
- 26:00377 so you have this 26.85 85 ohms and
- 26:05the impedance on the fundamental
- 26:07harmonic this will be equivalent to 6 +
- 26:11j xl-
- 26:14xc so you have this impedance 1
- 26:18equivalent to 6- g8 so meaning in the
- 26:22fundamental harmonic our circuit behaves
- 26:25as like a capacitor or rc so we can uh
- 26:32we can We now have an idea that in the
- 26:36fundamental harmonic our current is
- 26:39leading the voltage. No, since this is
- 26:43an RC it behaves like a capacit capacite
- 26:48RC circuit no so expressing this or
- 26:53taking
- 26:54the uh magnitude of
- 26:57this quantity so you have this
- 27:00equivalent to 10 ohms. So solving
- 27:04for the RMS value of current no in the
- 27:09fundamental harmonic so we will use the
- 27:11RMS value of voltage 100 / by the
- 27:15impedance no 10 so uh we have a value of
- 27:2110 amp so for
- 27:23power so we can use the formula I squ
- 27:27only the resistance will consume the
- 27:30real power
- 27:31watts so Use the current since this is a
- 27:34series circuit
- 27:37I s R so 100
- 27:42so we have a power in the fundamental
- 27:46harmonic equivalent to 600 watts and the
- 27:50voltage drop across the inductor in the
- 27:53fundamental
- 27:54harmonic so I times the inductive
- 27:59reactance which is 18.85
- 28:0285 so you will have 188.5
- 28:055 volts and the face angle no solving
- 28:10for the face anglea 1 so you will have r
- 28:16tangent so we just use the impedance
- 28:21triangle or we are solving the power
- 28:24factor on the fundamental harmonic so
- 28:28the resistance is
- 28:306 and inductive uh capacitive reactance
- 28:35of J8 -
- 28:38J8 so you will have
- 28:41this angle of impeda angle equivalent to
- 28:46- 53.1°
- 28:4912° so meaning in the fundamental
- 28:53harmony you will have the expression for
- 28:55current let us say
- 28:58I1 this will be equivalent
- 29:02to the RMS value of
- 29:05current this is equivalent to I mean the
- 29:08maximum 10
- 29:11s ro
- 29:132 sin
- 29:19of omega t.
- 29:22Okay. So let's analyze. No. As you can
- 29:26observe
- 29:27in our voltage source, our voltage V has
- 29:32a face angle of
- 29:34zero. Okay. Face angle of zero. So I
- 29:38will just write it here. So if we're
- 29:41going to plot it in
- 29:43our cartesian plane, so your voltage is
- 29:48located just in the origin V.
- 29:52No. So V maximum or the
- 29:57VRMS. Next your
- 30:01current is at angle 53. Since this is
- 30:07our circuit the fundamental harmonic
- 30:09behaves as an RC like an RC. So meaning
- 30:13current naglead siya sa voltage by this
- 30:17angle
- 30:1953.1. So meaning your current ay naad
- 30:24rin
- 30:25naka-allocate. So angle between your
- 30:27current and voltage
- 30:29is
- 30:3453
- 30:3512 degrees. So to express this current
- 30:41no to express the sinusidal equation for
- 30:43this current so the location of this
- 30:46current from the origin is
- 30:48at+
- 30:5153.32 so ito siya express as
- 30:5953.12° so this is your expression for
- 31:02your eye in the
- 31:04fundamental harmonic. So 10 ro 2 or just
- 31:09I is im sin omega t +
- 31:1453. 12. Okay. So we are not finished
- 31:18yet. So let's proceed to this next
- 31:20harmonic. So in our voltage source so
- 31:23the next harmonic is the third harmonic
- 31:26having a maximum value of
- 31:28voltage equivalent to 70.7.
- 31:33So to take the RMS value of the
- 31:36voltage. So we just divide the maximum
- 31:40by s root of
- 31:432 and our inductive reactance of course
- 31:47this will change because the angular
- 31:49frequency is changing. So our angular
- 31:54frequency now is 3 times the fundamental
- 31:59frequency. So we just multiply the
- 32:03XL1 3 at times 3 anghang omega. So
- 32:09therefore we have now our XL3 equivalent
- 32:12to 56.55 55 and also the uh the
- 32:18capacitive reactance no so if going to
- 32:22change the increase
- 32:24the uh value of angular frequency so our
- 32:29inductive capacitive reactance
- 32:32will be will decrease no so will
- 32:37decrease by the multiplying factor no if
- 32:42we are if we are multiplying the or
- 32:45increasing
- 32:46the uh angular frequency by a factor of
- 32:503 our induct in our capacitive reactance
- 32:53will decrease by 3 or divided by 3 so
- 32:59therefore our xc will be equivalent to
- 33:028.95 95 so kung nagliog
- 33:07moon
- 33:09so that xc is 1 /
- 33:152π
- 33:17fc or omega c 1 / omega
- 33:22c mas dali
- 33:261 / omega c and if we triple this omega
- 33:34No so making c as our c will not change
- 33:38or our capacitance will not change so
- 33:42the value of xc will just be divided by
- 33:453 or if we double
- 33:48the so if we double the value of our
- 33:52angular frequency so our our xc will
- 33:56divided by
- 33:572 okay
- 34:00so that is how you compute for the XC on
- 34:06this the next
- 34:07harmonics. Okay.
- 34:10So at
- 34:13solbonia impedance so impedance in the
- 34:16third harmonic will not be and our
- 34:19resistance will not change
- 34:22ha constant no because R is not a
- 34:26function
- 34:27of any quantity. So R is the function of
- 34:32uh the angular frequency. No so that is
- 34:37why even if uh in the fifth harmony
- 34:40fourth harmonic so I will our R will
- 34:44remains the
- 34:46same. Okay so substitute 6 + JXL - XC so
- 34:526 + J 47.6 6
- 34:57ohms. So in the third
- 35:00harmonic you can see that our impedance
- 35:05function behaves like an RL circuit. So
- 35:11we already have an idea that in the
- 35:14third harmonic our current eye now logs
- 35:18the voltage by a certain angle no
- 35:22logging naong current danhe. So at timan
- 35:26ha so taking the magnitude of this
- 35:30quantity so you will have this
- 35:3248.1 ohms and solving for the RMS value
- 35:36of current in the third harmonic.
- 35:39So voltage RMS div
- 35:42by and that magnitude of the impedance
- 35:47so na siya
- 35:511.04. Now solving for power in the third
- 35:55harmonic. So we will use the third
- 35:59harmonic current square times the value
- 36:02of resistance R. So naatay 6.48.
- 36:0848
- 36:10wats the third harmonic and also we can
- 36:13solve now for the voltage drop across
- 36:16the inductor in the third
- 36:19harmonic so we have 58.9 9 vol and
- 36:26solving also for the face angle or the
- 36:28factor
- 36:29angle so we will use the power or I mean
- 36:34the impedence triangle
- 36:38so for our impedence
- 36:42triangle so
- 36:44the real part will be the r which is 6
- 36:49and the inductive part or the reactive
- 36:53part will be
- 36:5856
- 37:0055. Okay. So taking the R tangent
- 37:04opposite over adjacent for the XL / R.
- 37:09So we have this R tangent equivalent
- 37:13to R tangent of
- 37:1547.6/ 6 equ to 82.8.
- 37:20So what does this
- 37:23imply? So same as what we did in the
- 37:26fundamental harmonic. No. Okay. I will
- 37:29erase
- 37:34this. Okay. So as you can
- 37:38see our voltage no if we look back in
- 37:43the previous slide. So our voltage B is
- 37:48at 30.
- 37:52de socated pos
- 37:5830 so meaning our voltage
- 38:02b let us
- 38:06say 30°
- 38:09from the
- 38:13origin and since in the third harmonic
- 38:17our current eye is logging the voltage
- 38:20by certain angle and that angle is this
- 38:23angle so our eye is located somewhere
- 38:31here the angle between our voltage and
- 38:33current is
- 38:40828 so therefore the distance of this
- 38:43current I from the origin will now be
- 38:45equivalent to 82.8-
- 38:498- 30. So this is equivalent
- 38:53to uh
- 38:5982.8
- 39:02828 - 30 so we
- 39:06have 52.8.
- 39:11So we can express
- 39:14the
- 39:16uh current in the third harmonic no so I
- 39:22sub
- 39:253. So this will be equivalent to so RMS
- 39:29s of 2. So 1.04
- 39:3304 ro
- 39:362 sin
- 39:38of so since this is in the third
- 39:41harmonic o third harmonic sa na omega t
- 39:46and kin siya naman siya paubos no
- 39:52pa-counterclockwise I mean pa-clockwise
- 39:55clockwise direction so meaning the angle
- 39:57is negative so-
- 40:03528°. So this is your expression for
- 40:06current in the third harmonic. So 1.04
- 40:10ro 2 sin of 3 omeg t -
- 40:1452.8. So we have we have the last
- 40:18harmonic in the fifth
- 40:21harmonic. So fifth harmonic.
- 40:25So in the fifth harmonic we have the
- 40:26current or our voltage equivalent to
- 40:2928.
- 40:3128. I will look back. So
- 40:3628.28 at
- 40:40-2. So 28.28. So solving for the RMS. So
- 40:45we divide it by s of 2 and our inactive
- 40:49reactance will multiply by 5 no
- 40:54multiplied by 5 and our capacitive
- 40:58reactance will be divided by 5 our
- 41:02fundamental capacitive reactance will be
- 41:04divided by 5 and our
- 41:07fundamental uh inductive reactance will
- 41:11be multiplied by
- 41:135 So solving for the impedance in the
- 41:17fifth harmonic. So naay 6 + JXL which is
- 41:2494.25- capacitive reactance which is
- 41:275.37 so we have 6 + J 88.88 88 ohms. So
- 41:34as you can observe that impedance in the
- 41:37fifth harmonic behaves like an RL
- 41:40circuit since this is positive so RL
- 41:44siya then expected na that it is
- 41:48expected that our current in the fifth
- 41:50harmonic logs the voltage by a certain
- 41:56angle since RL circuit the R circuit
- 42:01ising the voltage
- 42:03So taking the magnitude of this quantity
- 42:07have this 89
- 42:09ohms and solving for the current in the
- 42:12fifth
- 42:13harmonic. So just substitute we have now
- 42:16the voltage RMS div the impedance. So
- 42:21you will have RMS carmonic equivalent to
- 42:260.225.
- 42:30So solving for the
- 42:32power. So this is equivalent to the
- 42:35square of the current times the
- 42:38resistance. So therefore you will have
- 42:41you have now the value for power in the
- 42:43harmonic equ
- 42:46to304
- 42:48watts and also the voltage drop across
- 42:53the inductor in the fifth
- 42:56harmonic you will have current times XL.
- 43:00This is equivalent
- 43:02to 2 and for the face
- 43:07angle so for the face angle so the same
- 43:11so tangent of XL over R which is
- 43:16equivalent to 86.1°
- 43:191 de okay so solving for the total RMS
- 43:25current or the current that our ameter
- 43:28will be reading this will be equivalent
- 43:32to the square root
- 43:34of the RMS in the
- 43:38fundamental square plus RMS value in the
- 43:42third harmonic plus the RMS value in the
- 43:46fifth harmonic so namay mga y so just
- 43:50substitute 10 s + 1.04 s + 20
- 43:550.225 square so you will have the RMS
- 44:00value or the total current this will be
- 44:03equivalent to 10.05
- 44:0705 and for the power so we just sum up
- 44:11no all the power consumed on each
- 44:16harmonic so the first fundamental you
- 44:19have 600 the third harmonic you have 648
- 44:236.48 48 and the third harmonic uh we
- 44:27have a value of
- 44:2934304 so in all we have total power
- 44:34what's consumed is
- 44:37606 8 and of course the total inductive
- 44:42voltage in the inductor so same lang
- 44:46kuha gap on to RMS sa VL so this will be
- 44:49equivalent to
- 44:51VRMS VLMS S in the fundamental, VLRMS in
- 44:56the third and VLRMS in the fifth
- 45:01harmonic. So ay
- 45:04198.8
- 45:06volts. Now for the equation of current
- 45:09wave form no at siyang-create sa una.
- 45:14So for the current in the first
- 45:16fundamental harmonic so
- 45:20naay
- 45:22pare
- 45:24114.14 sin omega t + 53.2 So this is the
- 45:29equation no equation where current in
- 45:32the fundamental harmonic. In the third
- 45:34harmonic we have this
- 45:371.47 sin of 3 om t -
- 45:4352.8. And in the third
- 45:45harmonic I mean in the fifth
- 45:47harmonic so you'll have
- 45:50this root of 2 * 0.25 sin of 5 om t -
- 45:56106.1 1 equivalent to
- 46:01-0.318 sin of 5 omeg t- 100.1
- 46:10one negative siya
- 46:15soat so take note that our
- 46:19voltage has
- 46:22a maximum value of negative
- 46:2628 and located at -
- 46:3220°
- 46:35so dinis
- 46:40ne 20 or
- 47:0020
- 47:02and and since
- 47:04our circuit in the fifth harmonic
- 47:08behaves like an inductive RL
- 47:11circuit. So logging ang kurente. So the
- 47:15angle between your current and voltage
- 47:19will be equivalent to 86.1.
- 47:23So somewhere
- 47:27here so this will be equivalent
- 47:31to
- 47:3586
- 47:371 so your voltage here is ne
- 47:4728.28 Ayan 28 no? Ano ba
- 47:52'to? -
- 47:5528.
- 47:5628. So if you have this voltage negative
- 48:00of course your current will also be
- 48:01negative so negative
- 48:04ay sub
- 48:065. So this angle here is
- 48:1186.1 and the distance of your i5 from
- 48:14the origin will now be equivalent to
- 48:1686.1
- 48:1920. So the expression of your current
- 48:22will be equivalent to this
- 48:27ne 2 the maximum current which is
- 48:330.25 sin of 5 omeg t - 106 because 86.1
- 48:38+ 20 is
- 48:40106.1 so negative si ha so - 106.1
- 48:45or
- 48:48-0.318 sin 5 om t +
- 48:53106.1 and therefore the complete
- 48:56expression for your current will now be
- 48:58equivalent to I1 I3 +
- 49:02I5 so morning naasay one
- 49:07ah
- 49:1014.4 sin of 53.12 12 +
- 49:14247 sin of 3 omeg t -
- 49:1752.8 - sin 5 om t -
- 49:23106.1 or we can also express this
- 49:28quantity in the other direction and it's
- 49:31opposite direction.
- 49:33If we going to take the opposite of this
- 49:35I so location will now be here. So if
- 49:39this is
- 49:40negative
- 49:42vector opposite vector no so this act in
- 49:47this direction and its opposite will be
- 49:49negative of
- 49:50this
- 49:52direction. Yeah. If this is 106.1
- 49:58And this angle now will
- 50:00be so an so since this is 106.1 so kay
- 50:0890 so 106.1-
- 50:1190 angle and this angle is just equal to
- 50:14this
- 50:16angle this is theta of course this angle
- 50:20is theta so 106.1
- 50:241-
- 50:2590 this is equivalent
- 50:31to 16.1 no
- 50:3616.1 and this is 16.1
- 50:40also. So 90- 16.1 so makuha so
- 50:4990- 16.1
- 50:51So have
- 50:5473.9
- 50:57[Musika]
- 51:0073.9
- 51:0273.9° so that is why we also have here
- 51:04another expression equivalent to and
- 51:07positive na ha I is positive so pos
- 51:120.318 318 plus ano positive
- 51:17+318 sin of 5 omeg t + 73.9 9 amp. So
- 51:22this is the complete expression for the
- 51:25current or you can also you can can have
- 51:27your answer as
- 51:30kanilang
- 51:33no pwede
- 51:36na
- 51:38kanya or pwede po kini i answer si ha.
- 51:44Okay. So, okay. So, so let's proceed to
- 51:47another
- 51:49example. So, this is we will now be
- 51:52having an example for a parallel. So,
- 51:55that's for series in the
- 51:57previous sa parallel. So, for example,
- 52:00given a circuit shown in figure 23 with
- 52:0460 cycle constant as
- 52:06shown 60 cycle 60 herz. So when the
- 52:10voltage
- 52:13V when the voltage V is equivalent to
- 52:16141.4 sin omega t + 7 sin omega t in the
- 52:21fundamental
- 52:23harmonic
- 52:25and in the third
- 52:27harmonic naatay
- 52:3170.7 plus 30 it's face angle is 30 and
- 52:34the third harmonic I mean in the fifth
- 52:36harmonic - 28.28 28 sin 5 om t -
- 52:4120 find the ameter value of the total
- 52:45current i
- 52:48so the reading of our ameter the current
- 52:52in each branch power dissipated by each
- 52:56branch total power dissipated and the
- 52:59equation of the resultant
- 53:01current so our omega or our angular
- 53:04frequency will be equivalent to 377 7
- 53:08radians per seconds. So this is our
- 53:12circuit no parallel branches. So RC 5
- 53:17ohms and 15 ohms. 5 ohms ang R C is 15.
- 53:22And R in the second branch connected by
- 53:26CD point CD. So 10 ohm resistance and 2
- 53:30ohms inductive reactance. Okay. So let's
- 53:34now solve for
- 53:36the um anouns nouns quantity. So as what
- 53:42the same as what we did on the previous
- 53:45example so in solving for a parallel
- 53:49same procedure lang. Soccerons ang iyang
- 53:53mga components. So for first solve for
- 53:56the fundamental component second in the
- 53:59third component or whatever component is
- 54:02present.
- 54:03And the last is the last third component
- 54:06or fifth fifth harmonic. Soon
- 54:10lang depende na kung voltage source or
- 54:14even current source kung upat siya na si
- 54:16harmonic 7 so kaupat po ka or kalima po
- 54:21ka mo mag-solve consider good mo kada
- 54:24component or kada harmonic. So first
- 54:27move si ka sa fundamental.
- 54:31So in the fundamental
- 54:33harmonic angipangita niya is ang current
- 54:37voltage sa power no total
- 54:42power so in the fundamental harmonic our
- 54:45voltage or our maximum voltage is 141.4
- 54:504 so divide siya 2 para makuha na to ang
- 54:55iyahang ah iyahang RMS value. So 100 +
- 55:03J0 ang voltage
- 55:07sa RM voltage sa fundamental. So current
- 55:11in the first branch can see in the first
- 55:19branch so to solve for the current in
- 55:21the first branch we need the impedance
- 55:23in the first branch so namay voltage
- 55:27100/ impedance ng 5- j15 so in the
- 55:30fundamental harmonic mam itong value
- 55:33na
- 55:35j15 or - j15 minus kay capacitor 1. So
- 55:41in the first branch we have a current
- 55:44of 2 + J0 or 2
- 55:50amp. So currents in the second
- 55:54branch or in the CD branch
- 55:58kini. So voltage divided by impedance
- 56:0110. So iyung quantity iyang value sa
- 56:03impedance is 10 + J2.
- 56:07So that is why
- 56:08100/ 10 + J2. So result niya is
- 56:139.62- J
- 56:161.925. So taking the magnitude of this
- 56:19current so naay
- 56:239.82
- 56:25amp. So next atong ang total in the
- 56:30fundamental.
- 56:32So total niya ang total current is
- 56:35just summation of the current on each
- 56:39branch
- 56:40parallel current plus current current in
- 56:43the fundamental harmonic. So that is
- 56:47IAB1
- 56:48plus
- 56:50ICD
- 56:521.
- 56:54Okay. So our current therefore will be
- 56:57equivalent to this quantity 12.323
- 57:0333.
- 57:06Okay. Next. Solve for the face
- 57:11angle. So how to solve for the face
- 57:14angle? So siya. So at kuha iyahang
- 57:19equivalent
- 57:21ng pwede lang gamit an current no. So
- 57:25real
- 57:29uh current the real component is
- 57:31equivalent to
- 57:3611.62 iyahang imaginary component kanina
- 57:40J
- 57:41ngang
- 57:454.075 so nag tangent ha r tangent of
- 57:494.075 / 911.62
- 57:5362 so naay angle equivalent to
- 57:5919
- 58:014 okay so next solve for the power in
- 58:05the first branch so naman tay current
- 58:09diha so
- 58:13power this will be equivalent
- 58:18to okay real naman eh wajer component so
- 58:21pwede lang anim ah the real part times
- 58:25the voltage so natay 200 watts and also
- 58:30in the second branch CD branch so 100
- 58:34voltage times 9.62
- 58:3662 real component. So pwede lang na
- 58:40gamitan 962 wats
- 58:44ng ah power in
- 58:48the second branch on the
- 58:51fundamental harmonic.
- 58:54Sunod and the third harmonic. So third
- 58:58harmonic our na our frequency or angular
- 59:03frequency 3 no so mahitabo ang
- 59:09XC maivide by 3 while our inductance or
- 59:15our inductive reactance XL ma-multiply
- 59:18by 3. So RMS value in our kuan sa volt
- 59:25in the third harmonic so naay 50 volts
- 59:30or express in kuan in rectangular
- 59:33coordinates of 50 + J0 imaginary
- 59:38component and solving for the current in
- 59:40the AB branch in the third harmonic soay
- 59:4550 volts div 5-
- 59:49j5 so 5 +
- 59:52J 5 so magnitude nga 7.07
- 1:00:0007 so in the CD branch 10 +
- 1:00:04J at 50/ 10 + J6 so
- 1:00:09na value 3.68 - J
- 1:00:152.21 in the so iang magnitude naay 4.33
- 1:00:20so atong i-adding du ha vector addition
- 1:00:23ha so 5 + 3.68 68 naay
- 1:00:278.68 and 5
- 1:00:31J5 - J2.21 so naay 2.79 so iyahang
- 1:00:36magnitude
- 1:00:399.11 so kung ano to
- 1:00:42i-angle so kani lang ah the imaginary
- 1:00:45component divided by the real component
- 1:00:48soay 17.85
- 1:00:5385 de so the same to solve for the power
- 1:00:58gamit real
- 1:01:00component 5 voltage
- 1:01:0550 then voltage ng 50 times sa real
- 1:01:08components ng current ng branch 3.68 68
- 1:01:14so ay
- 1:01:16184 watts so muna siya for the third
- 1:01:21harmonic next last harmonic fifth
- 1:01:24harmonic so nahimong times 5 ang omega
- 1:01:30no soong current or
- 1:01:37voltage so
- 1:01:39rms 20 or
- 1:01:43orang
- 1:01:45voltage equivalent to in terms of ah in
- 1:01:50terms of tangular 20 +
- 1:01:54j and
- 1:01:56karon ayahan ng ayaahan naing kuan
- 1:01:59ayahan naing xc ma-divide by 5 gikan si
- 1:02:04ang fundamental ang fundamental is 15
- 1:02:08man 5 so thatay Sorry ohms ah nahiya
- 1:02:13hading ko an indu uh inductive inductive
- 1:02:18reactance ma-multiplied by 5 so
- 1:02:23naay 10 ohms so the same procedure solve
- 1:02:28ka sa current in the first branch so RMS
- 1:02:32voltage divided by current naatay ken
- 1:02:352.94 + J.76 76
- 1:02:39763 then taking its magnitude you have
- 1:02:43this 3.43 amp and the next branch CD
- 1:02:47branch so again 20/ 10 + J10 so ayusan
- 1:02:54mo i-mine ang negative
- 1:02:56haon ang k lang nagdetermin n direction
- 1:03:00ha ayaw siya na i-mind only magnitude
- 1:03:02sa so naatay 1- j1 or 1.414
- 1:03:07414 i-add na to ang duha ka current king
- 1:03:11mga current din i-add para makuha na to
- 1:03:13diha in the fifth sa fifth
- 1:03:15harmonic so
- 1:03:17naatay current nga 3.94 +
- 1:03:23j.63 or
- 1:03:254.01 amp so solving for its angle tayo
- 1:03:3010.95
- 1:03:3395° so solving for the
- 1:03:36power so voltage times the real
- 1:03:39component of
- 1:03:41current so 58 and 20 plus 1 only 20 wats
- 1:03:49so sunod ito na kuha
- 1:03:52total so the amity reading is ma ang
- 1:03:55total current at point f so total
- 1:03:59current is the fundamental
- 1:04:0112 point or it's RMS value
- 1:04:0412.33 plus the RMS value of current
- 1:04:08in the third harmonic square plus the
- 1:04:11third or the RMS value of current in the
- 1:04:16fifth harmonics. All in all naay 15.9
- 1:04:20ang maasa sa atong ameter so sa kada
- 1:04:24branch sad so at
- 1:04:27gamitan square root of RMS value of
- 1:04:30current in the first
- 1:04:32branch plus the square of the arm's
- 1:04:36value of current in the second branch
- 1:04:37plus the arm's value of current in the
- 1:04:39third branch square. So naay 10.1 one
- 1:04:42and last in the CD
- 1:04:45branch mga values
- 1:04:47balik so
- 1:04:50value so sa first
- 1:04:54branch first
- 1:04:56branch first
- 1:05:02branch
- 1:05:10Okay. So the total power ato lang
- 1:05:13ipang-sum tanan in the first branch plus
- 1:05:18tan i-add na to sa second branch cd
- 1:05:21branch i-add tanan. So ang total
- 1:05:25niya plus power AB plus power CD have
- 1:05:30this
- 1:05:32quantity. Now sa current wave form
- 1:05:36current wave form the fundamental
- 1:05:39branch
- 1:05:43so ah balik ha. So in the fundamental
- 1:05:47branch so diha current kini 12.33
- 1:05:5233
- 1:05:54okay 12.33 33 maxim RMS na times na to
- 1:05:59sa iyang s of 2 para makuha tag im in
- 1:06:02the first branch or i mean in the
- 1:06:04fundamental component so sin omega t +
- 1:06:1019
- 1:06:1244 so kung imohang kuanon kung imohang
- 1:06:16solbon ang total impedance sa
- 1:06:18circuit considering the
- 1:06:21fundamental
- 1:06:22component so diha na makita Kung un sa
- 1:06:27ato ang
- 1:06:27circuit it could be RL or RC. So let's
- 1:06:34check para dali lang. So ato ang formula
- 1:06:37na parallel
- 1:06:39lang itong parallel or pwede to in terms
- 1:06:42of admittance no pwede tay in terms of
- 1:06:46admittance if daghan na siyang branches
- 1:06:49or pwede sad
- 1:06:51duhara para ato lang gamitan
- 1:06:57formula sa parallel ng dua branch lang
- 1:07:00du ka branches so as you can see that
- 1:07:05Our
- 1:07:07equivalent impedance in the fundamental
- 1:07:10component is equivalent to 7.66 - J
- 1:07:182.69. Okay. So un na siya so
- 1:07:22RC no behaves like a capacitive branch.
- 1:07:29So take note that our voltage in the
- 1:07:32fundamental na lang siya sa origin
- 1:07:36zero angle so siya leading
- 1:07:42current so expected that our i is
- 1:07:45somewhere above our
- 1:07:47vle between moto nacompute ito sa i
- 1:07:53194 so that is why the equation for
- 1:07:56current in the fundamental branch
- 1:07:59naay k r value in the
- 1:08:02fundamental 2 cos of omega t plus the
- 1:08:06distance sa i from the origin 19.4
- 1:08:10or siya in the third
- 1:08:13harmonic o same procedure so kamay
- 1:08:17bahala mo na mo ah compute check lang
- 1:08:22check so naay procedure ako
- 1:08:25nag-introduce previously so just learn
- 1:08:29from it and also in the fifth harmonic
- 1:08:33ma so review mo naing siya so finally
- 1:08:37equation for current
- 1:08:40So you will now have the equation for
- 1:08:43current equivalent
- 1:08:46to ah
- 1:08:4917.45
- 1:08:51+ ah sin omega t + 19.4 + 12.9 sin 3
- 1:08:56omeg t + 47.85 85 +
- 1:09:035.67 sin 5 omeg 3 +
- 1:09:08171°. Okay. So that would be all for our
- 1:09:13discussion. So I hope you learn
- 1:09:15something and if you are if you have any
- 1:09:19question so just drop a message on
- 1:09:24my social media account.
- 1:09:29Okay. So that concludes our discussion
- 1:09:33on the RMS value of nonsenosoidal waves.
- 1:09:37So understanding how to compute and
- 1:09:39interpret RMS values equip us to work
- 1:09:43with real world signals.
- 1:09:46system
- 1:09:47efficiency and ure safety and accuracy
- 1:09:51in electrical circen
- 1:09:55M.
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