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RMS VALUE OF NON SINUSOIDAL WAVE — Transcript

by Lizandro Bitang · 6,535 words · 1,138 segments · language en · Watch on YouTube

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  1. 0:01Good day everyone. So welcome to our to
  2. 0:05the continuation of our
  3. 0:08discussion on the topic
  4. 0:11nonosoidal waves. So I really now
  5. 0:15excited to guide you through the topic
  6. 0:19that plays a vital role in modern
  7. 0:23electrical
  8. 0:24engineering. So this is the RMS or the
  9. 0:27effective value of the sinusoidal wave
  10. 0:31form. So in this
  11. 0:33presentation we go beyond the typical
  12. 0:35side wave and explore how to deal with
  13. 0:38real world signals which are of
  14. 0:41irregular and complex in shape. So let's
  15. 0:46begin.
  16. 0:52So in electrical engineering the
  17. 0:55effective value or the RMS or root
  18. 0:58square is used to express an alternating
  19. 1:03quantity in terms of its equivalent DC
  20. 1:08value particularly in how it delivers
  21. 1:11power to a resistive load while senosal
  22. 1:17wave form are often used in theory and
  23. 1:20textbooks. Most practical signals like
  24. 1:23those found in power electronics and
  25. 1:26digital systems are nonsenosidal.
  26. 1:30So for example we have this square waves
  27. 1:34triangular
  28. 1:36waves and complex distorted signals.
  29. 1:40That is why understanding how to compute
  30. 1:45RMS values for such wave forms is both a
  31. 1:48theoretical necessity and a practical
  32. 1:55skill. So let's define it formally. The
  33. 1:59root means square value of a periodic
  34. 2:01wave form is equivalent to the square
  35. 2:04root of the
  36. 2:06average of the squares of the
  37. 2:08instantaneous values over one cycle. So
  38. 2:13we will just we will use this formula
  39. 2:18no. So why is the RMS
  40. 2:24value? This is because it reflects the
  41. 2:28true power capability of an AC source.
  42. 2:33In resistive
  43. 2:34circuits, it determines how much thermal
  44. 2:38energy will be generated.
  45. 2:40Whether we analying power supplies,
  46. 2:44motors and communication signals, RMS
  47. 2:48provides a consistent and comparable
  48. 2:52measure of
  49. 2:54energy. In essence, it gives us a fair
  50. 2:58comparison between AC and
  51. 3:02DC power.
  52. 3:09So now let's explore the core of our
  53. 3:12topic. How to calculate RMS for
  54. 3:17nonsenosoidal wave form. Unlike pure
  55. 3:20sinusoids, nonsinosoidal signals may
  56. 3:23contain multiple harmonics or follow
  57. 3:26shapes like square or triangular
  58. 3:30patterns. So for example we have the
  59. 3:33square wave. So to compute for the
  60. 3:35amplitude or I mean for the RMS value of
  61. 3:40this wave. So we have here the piece
  62. 3:44wise function. So for
  63. 3:47example you have this square wave no
  64. 3:51from 0 up to time t for one full cycle
  65. 3:56or one period. So labeled as T sub O. So
  66. 4:01half of it will be equivalent to t / 2
  67. 4:06and the other half is t / 2. So for the
  68. 4:10first function from
  69. 4:130 to t / 2 you have this a no equation a
  70. 4:20from 0 to t / 2 and from t / 2 to t so
  71. 4:27you have this -
  72. 4:30a just substitute this to our
  73. 4:34formula okay so for the full cycle for
  74. 4:37one cycle of the wave
  75. 4:39have this the positive cycle plus the
  76. 4:42negative RMS of the negative cycle. So
  77. 4:46after manipulating the
  78. 4:48integral so come up with the value of
  79. 4:51the RMS of a square wave equivalent to
  80. 4:56its
  81. 4:58amplitude. Next.
  82. 5:02So for a triangular wave having a pick
  83. 5:04value of a so RMS value is equivalent to
  84. 5:08the amplitude divided by s root of 3. So
  85. 5:14the derivation of this formula will be
  86. 5:17left as your
  87. 5:20exercise. And also for a soot wave for a
  88. 5:24pick value of a
  89. 5:26again so we have a value of a divided by
  90. 5:30s root of 3. So take note of this
  91. 5:35quantities or
  92. 5:40equations. So for a general complex wave
  93. 5:43so the instantaneous current as a for
  94. 5:45example this instantaneous current as a
  95. 5:48function of time. So this is composed of
  96. 5:52several harmonics no so they have
  97. 5:55fundamental second third up to and
  98. 5:59harmonic so a sub0er here represents the
  99. 6:02dc component so im1 im2 im3 imn are the
  100. 6:09maximum values of each harmonic and
  101. 6:14alpha 2 alpha 3 are the face angl
  102. 6:20and omega is our angular frequency and t
  103. 6:24represents the time.
  104. 6:28So let's solve for or let's find a
  105. 6:32formula in solving for the RMS value of
  106. 6:37this complex wave.
  107. 6:41So we will just use the formula for
  108. 6:46solving the RMS value. So we just
  109. 6:49substitute the instantaneous value or
  110. 6:52the instantaneous
  111. 6:53equation. So you have this quantity
  112. 6:57square dt from 0 to t for one period or
  113. 7:03for one whole cycle.
  114. 7:05So after manipulating this integral so
  115. 7:09come up with this effective value or RMS
  116. 7:12value equivalent
  117. 7:13to square root of the DC component squ
  118. 7:16plus the summation of the individual
  119. 7:19maximum value on each harmonic and
  120. 7:23squares so divided by
  121. 7:262 and also we can express that equation
  122. 7:30in terms of RMS value of each harmony.
  123. 7:35Okay.
  124. 7:38So uh take note that RMS is equivalent
  125. 7:41to the maximum value divided by SO 2 for
  126. 7:45aign wave. Ha? This is just applicable
  127. 7:47for a sign
  128. 7:49wave. So I over s root of 2. So
  129. 7:55substituting this value to the equation
  130. 7:58previous equation. So we arrive on
  131. 8:02this uh formula for RMS value in terms
  132. 8:06of the RMS value of each
  133. 8:10harmonic. Okay. So we can also use this
  134. 8:13formula if you are solving for harmonic
  135. 8:16of each uh RMS value of harmonic so you
  136. 8:19can use this formula.
  137. 8:26And also we can also solve for the power
  138. 8:30no power due to
  139. 8:32anosidal voltage so we have here the
  140. 8:35general expression for the average
  141. 8:37power in a circuit with time varying
  142. 8:41voltage and current given as this
  143. 8:43equation.
  144. 8:45So I already introduced this equation to
  145. 8:48you in our previous
  146. 8:50discussions. 1 / t integral of e of t or
  147. 8:55the instantaneous value of voltage times
  148. 8:57instantaneous value of current dt over 1
  149. 9:01period from 0 to t.
  150. 9:05So for example if you have
  151. 9:08this nonsusidal voltage oranous voltage
  152. 9:12equivalent is em sub 1 sin omega t +
  153. 9:16alpha 1 + em sub 2 sin 2 omeg t so and
  154. 9:19so forth and for
  155. 9:22current im sub 1 sin omega t + alpha 1
  156. 9:26prime 1. So we just substitute
  157. 9:30this uh equations to our formula for
  158. 9:36power then integrate it from 0 to t for
  159. 9:40one period. So after integrating the
  160. 9:44equation or the
  161. 9:47integral so we come up with this formula
  162. 9:51for power. So is this is this is just a
  163. 9:55summation of uh its maximum product of
  164. 10:00maximum value of each harmony divided by
  165. 10:042 and cosine of the difference of the
  166. 10:07two phase
  167. 10:09angles. So em sub 1 and im sub one
  168. 10:12corresponds to the fundamental harmonic
  169. 10:14and you will also use the uh face angle
  170. 10:18of its harmonic of fundamental harmonic.
  171. 10:22So for voltage you have alpha 1 and for
  172. 10:25current alpha prime
  173. 10:281. Every everything will just
  174. 10:32follow. So take note of the
  175. 10:39formula. So to to better understand our
  176. 10:43formula. So let's apply it to our
  177. 10:46example. So find the power represented
  178. 10:49by the following
  179. 10:52given. So instantaneous voltage
  180. 10:54equivalent to 100 sin omega t + 30 - 50
  181. 11:00sin 3 om t + 60. So 25 + 5 sin 5 omeg t
  182. 11:08and for current 20 sin omega t - 30 + 15
  183. 11:13sin 3 om t + 30 + 10 cos 5 omeg t - 60
  184. 11:19amp. So we have now this
  185. 11:22two uh instantaneous values of voltage
  186. 11:26and current. So for the voltage it is
  187. 11:30expressed in terms of a sign function
  188. 11:33and for current
  189. 11:36so expressed in sign and the fifth
  190. 11:40harmonic is expressed in terms of
  191. 11:44cosine. So before solving or before
  192. 11:47applying the formula see to it that the
  193. 11:50quantities
  194. 11:51are consistent. So meaning if in the
  195. 11:55fifth
  196. 11:56harmonic you are using sign of course in
  197. 11:59the fifth harmonic of the instantaneous
  198. 12:03current it should also be sign so we
  199. 12:08convert this function or this equation
  200. 12:10in terms of
  201. 12:13sin so recall the formula that
  202. 12:19cosθ is equivalent
  203. 12:22to sin
  204. 12:26ofθa +
  205. 12:3190°. Okay. So
  206. 12:36substitute sin
  207. 12:38of 5 omeg
  208. 12:43t -
  209. 12:4660 + 90.
  210. 12:51So this quantity 10 cos 5 omeg t- 60° is
  211. 12:55equivalent to
  212. 12:5810 sin
  213. 13:02of
  214. 13:045 omega
  215. 13:10t
  216. 13:13plus 30.
  217. 13:15Okay. So this this is the equivalent sin
  218. 13:19of this cosine quantity. So we can now
  219. 13:23use the formula.
  220. 13:27Okay. So, so for for the fundamental
  221. 13:30harmonic so the maximum value for
  222. 13:33voltage is 100 times the maximum value
  223. 13:36for current 20/ 2 cos of the face angle
  224. 13:41of the voltage which is 30
  225. 13:45minus cos uh minus the face angle of the
  226. 13:48current which is nega 30.
  227. 13:53Next for in the third
  228. 13:56harmonic so will have
  229. 13:59-50
  230. 14:0115/ 2 cos of the face angle of the
  231. 14:06voltage the third harmonic which is
  232. 14:0960 min the face angle of
  233. 14:15the current the harmonic 30 and in theth
  234. 14:20harmonic
  235. 14:22So we have this maximum value of
  236. 14:2525
  237. 14:2710/ 2 cos of the face angle of the fifth
  238. 14:32harmonic is zer so 0 min the face angle
  239. 14:38of the third harmonic which
  240. 14:40is I mean in the fth harmonic which is
  241. 14:4430
  242. 14:46so after substituting the vales
  243. 14:50No. So you can now solve for by
  244. 14:54using your calculators. You can solve
  245. 14:57for current or the power I
  246. 15:00mean.
  247. 15:01Okay. So for this quantity you have this
  248. 15:06500 watts. And for the next quantity for
  249. 15:11the third harmonic you have - 324.75 75
  250. 15:15and for the fifth harmonic you will have
  251. 15:18108.25
  252. 15:2025. So summing up all of this will
  253. 15:25result to the power which is equivalent
  254. 15:29to
  255. 15:33283.5. Okay. So let's proceed to the
  256. 15:40next. So we have here another example.
  257. 15:44So find the power delivered by the
  258. 15:48following instantaneous values of
  259. 15:51voltage and current.
  260. 15:54So you have here for the voltage you
  261. 15:56have a value 100 sin omega t + 50 sin 5
  262. 16:01omeg t- 80- 40 cos and for the current
  263. 16:07we have 30 sin of omeg t +
  264. 16:1160 sin of 5 omeg t - 50 and sin 7 10 sin
  265. 16:177 omeg t + 60 so as you can observe that
  266. 16:23the seventh harmonic for the voltage
  267. 16:25source is expressed in terms of cosine.
  268. 16:30So we convert this into sin. Okay. So s
  269. 16:36function so step one we have here
  270. 16:39convert all to sign function. So the -
  271. 16:4240 cos 7 om t + 30 is equivalent to in
  272. 16:47terms of s this is equivalent to
  273. 16:50-47 omeg t +
  274. 16:5520°. So solving for the
  275. 16:58power same as what we did on the
  276. 17:00previous
  277. 17:02example solve for the
  278. 17:05individual power on
  279. 17:07its harmonic. So in the fundamental
  280. 17:11harmonic you have here 100
  281. 17:1530/ 2 cosine of so your face angle for
  282. 17:20the fundamental harmonic of your voltage
  283. 17:23is
  284. 17:24zero and for your current is 60 so 0-
  285. 17:2960 so using using your
  286. 17:33calculator so you will come up of this
  287. 17:36on this value of 750 50 wat and next in
  288. 17:41the fifth harmonic you have
  289. 17:44433 and in the 7th harmonic you
  290. 17:47have 100 so take the sum of this three
  291. 17:52powers no so you come up with this value
  292. 17:58of value of power which is equivalent
  293. 18:08So ah
  294. 18:13okay this value of
  295. 18:22sorry
  296. 18:27okay so volt ampires or your
  297. 18:34uh apparent power and power factor for
  298. 18:38nonosidal waves. So the volt amper
  299. 18:41apparent for the apparent power. So volt
  300. 18:44amper so this is determined by the
  301. 18:46product of the effective voltage and the
  302. 18:48effective current.
  303. 18:50So you are already familiar with
  304. 18:54it that S or the apparent power is
  305. 18:57equivalent
  306. 18:59to the voltage times the current SBI. So
  307. 19:05this is in
  308. 19:08terms for the volt
  309. 19:10amper we just use this formula. So take
  310. 19:15the RMS value of the voltage no and also
  311. 19:19take the RMS value of the
  312. 19:21current and multiply
  313. 19:25it. So for
  314. 19:27example so in our previous
  315. 19:29example you have here the
  316. 19:33the RMS value for
  317. 19:36voltage and RMS value for current. So
  318. 19:39just take the RMS value of each
  319. 19:41quantity.
  320. 19:43Sige. So, so you have here the value
  321. 19:49for it's a parent power equivalent to
  322. 19:5510001
  323. 19:56vol. So just take
  324. 19:59the uh RMS value of the voltage and the
  325. 20:03RMS value of the current and multiply
  326. 20:07them will have the amp the apparent
  327. 20:12power.
  328. 20:14Next. So for the power factor so power
  329. 20:18factor this is the ratio
  330. 20:23between ratio between the real power and
  331. 20:26the apparent power. So this is a measure
  332. 20:30of how much real power has been consumed
  333. 20:34for the given apparent power. Okay. So
  334. 20:39you just substitute the formula. So this
  335. 20:41is the formula for the real power p no
  336. 20:46real power p
  337. 20:49and the denominator is the apparent
  338. 20:58power so this is p or
  339. 21:03div va
  340. 21:06or vol ampes
  341. 21:12So for example in our previous example
  342. 21:15in example 6 so we compute we computed
  343. 21:19this equivalent wats no power and in our
  344. 21:23prev example 7 so we computed
  345. 21:27this volt amp the apparent so just
  346. 21:31divide
  347. 21:32p
  348. 21:34va come up with this with this this
  349. 21:38value
  350. 21:39of our
  351. 21:43factor. So na siya no ratio between the
  352. 21:49real power and the apparent
  353. 21:56power. Okay. So let's now come to
  354. 21:59circuit analysis when waves are
  355. 22:02nonsenosoidal.
  356. 22:04So we just walk through on this example
  357. 22:07to better understand how we're going to
  358. 22:09analyze a
  359. 22:11circuit when our source source voltage
  360. 22:16and current are expressed in
  361. 22:21nonosoidal. So for
  362. 22:23example given the circuit with the
  363. 22:26parameter shown
  364. 22:30so these are the parameters of our
  365. 22:33circuit. So a series
  366. 22:35circuit no so when omega or the angular
  367. 22:38frequency is 377 radians per second and
  368. 22:43the voltage source is
  369. 22:45141.4 sin omega t + 70.7 sin 3 om t +
  370. 22:5130° - 28.28 28 sin 5 omeg t-
  371. 22:5620° volt is impressed.
  372. 23:00find the current I so the reading if you
  373. 23:04have if you connect here an
  374. 23:08ameter that ameter would read and also
  375. 23:11find the total power dissipated and the
  376. 23:15effective value of voltage drop across
  377. 23:18the inductance and also find the
  378. 23:21equation for the current wave so to
  379. 23:27solve this problem no uh we will
  380. 23:30consider the current on each fonda on
  381. 23:36each on each harmonic. So for let's
  382. 23:39first analyze using the fundamental
  383. 23:41harmonic and second let's analyze the
  384. 23:45current or the voltage drop in the third
  385. 23:49harmonic and also in the fifth harmonic.
  386. 23:54So first let's do the analysis in the
  387. 23:58fundamental harmonic. So we have the
  388. 24:00given. So you have R equ to 6 ohms L
  389. 24:050.05 Henry and 98.8
  390. 24:09microfarad. Then the source voltage is
  391. 24:13given. So what we are going to solve is
  392. 24:17the current
  393. 24:18I the total power dissipated effective
  394. 24:21value for voltage drop across the
  395. 24:24inductor and in equation of the current
  396. 24:28wave. So take note that the ameter would
  397. 24:30only read
  398. 24:32RMS value ha the effective
  399. 24:35value. That's what our ameter would
  400. 24:39read. So first let's analyze the circuit
  401. 24:43in the
  402. 24:45fundamental harmonic. Okay. So
  403. 24:49fundamental
  404. 24:50harmonic. So you have your voltage
  405. 24:52number one equivalent
  406. 24:55to so in the fundamental harmonic. So
  407. 24:58you have this value
  408. 25:00of your voltage maximum
  409. 25:04141.4. So ah let's solve for its RMS
  410. 25:09value. So we will divide it by root of 2
  411. 25:14since this is expressed in sign. So
  412. 25:16141.4
  413. 25:174
  414. 25:192 100
  415. 25:23volt inductance in the fundamental
  416. 25:25harmonic so we will use the omega
  417. 25:28equivalent to
  418. 25:32377 this is because in the fundamental
  419. 25:36harmonic you have your angular frequency
  420. 25:38as
  421. 25:41omega okay so 377 times the inductance
  422. 25:45you have this
  423. 25:4718.85 ohms and for your capacitance or
  424. 25:51capacitive reactance again use
  425. 25:55the
  426. 25:57value of omega to
  427. 26:00377 so you have this 26.85 85 ohms and
  428. 26:05the impedance on the fundamental
  429. 26:07harmonic this will be equivalent to 6 +
  430. 26:11j xl-
  431. 26:14xc so you have this impedance 1
  432. 26:18equivalent to 6- g8 so meaning in the
  433. 26:22fundamental harmonic our circuit behaves
  434. 26:25as like a capacitor or rc so we can uh
  435. 26:32we can We now have an idea that in the
  436. 26:36fundamental harmonic our current is
  437. 26:39leading the voltage. No, since this is
  438. 26:43an RC it behaves like a capacit capacite
  439. 26:48RC circuit no so expressing this or
  440. 26:53taking
  441. 26:54the uh magnitude of
  442. 26:57this quantity so you have this
  443. 27:00equivalent to 10 ohms. So solving
  444. 27:04for the RMS value of current no in the
  445. 27:09fundamental harmonic so we will use the
  446. 27:11RMS value of voltage 100 / by the
  447. 27:15impedance no 10 so uh we have a value of
  448. 27:2110 amp so for
  449. 27:23power so we can use the formula I squ
  450. 27:27only the resistance will consume the
  451. 27:30real power
  452. 27:31watts so Use the current since this is a
  453. 27:34series circuit
  454. 27:37I s R so 100
  455. 27:42so we have a power in the fundamental
  456. 27:46harmonic equivalent to 600 watts and the
  457. 27:50voltage drop across the inductor in the
  458. 27:53fundamental
  459. 27:54harmonic so I times the inductive
  460. 27:59reactance which is 18.85
  461. 28:0285 so you will have 188.5
  462. 28:055 volts and the face angle no solving
  463. 28:10for the face anglea 1 so you will have r
  464. 28:16tangent so we just use the impedance
  465. 28:21triangle or we are solving the power
  466. 28:24factor on the fundamental harmonic so
  467. 28:28the resistance is
  468. 28:306 and inductive uh capacitive reactance
  469. 28:35of J8 -
  470. 28:38J8 so you will have
  471. 28:41this angle of impeda angle equivalent to
  472. 28:46- 53.1°
  473. 28:4912° so meaning in the fundamental
  474. 28:53harmony you will have the expression for
  475. 28:55current let us say
  476. 28:58I1 this will be equivalent
  477. 29:02to the RMS value of
  478. 29:05current this is equivalent to I mean the
  479. 29:08maximum 10
  480. 29:11s ro
  481. 29:132 sin
  482. 29:19of omega t.
  483. 29:22Okay. So let's analyze. No. As you can
  484. 29:26observe
  485. 29:27in our voltage source, our voltage V has
  486. 29:32a face angle of
  487. 29:34zero. Okay. Face angle of zero. So I
  488. 29:38will just write it here. So if we're
  489. 29:41going to plot it in
  490. 29:43our cartesian plane, so your voltage is
  491. 29:48located just in the origin V.
  492. 29:52No. So V maximum or the
  493. 29:57VRMS. Next your
  494. 30:01current is at angle 53. Since this is
  495. 30:07our circuit the fundamental harmonic
  496. 30:09behaves as an RC like an RC. So meaning
  497. 30:13current naglead siya sa voltage by this
  498. 30:17angle
  499. 30:1953.1. So meaning your current ay naad
  500. 30:24rin
  501. 30:25naka-allocate. So angle between your
  502. 30:27current and voltage
  503. 30:29is
  504. 30:3453
  505. 30:3512 degrees. So to express this current
  506. 30:41no to express the sinusidal equation for
  507. 30:43this current so the location of this
  508. 30:46current from the origin is
  509. 30:48at+
  510. 30:5153.32 so ito siya express as
  511. 30:5953.12° so this is your expression for
  512. 31:02your eye in the
  513. 31:04fundamental harmonic. So 10 ro 2 or just
  514. 31:09I is im sin omega t +
  515. 31:1453. 12. Okay. So we are not finished
  516. 31:18yet. So let's proceed to this next
  517. 31:20harmonic. So in our voltage source so
  518. 31:23the next harmonic is the third harmonic
  519. 31:26having a maximum value of
  520. 31:28voltage equivalent to 70.7.
  521. 31:33So to take the RMS value of the
  522. 31:36voltage. So we just divide the maximum
  523. 31:40by s root of
  524. 31:432 and our inductive reactance of course
  525. 31:47this will change because the angular
  526. 31:49frequency is changing. So our angular
  527. 31:54frequency now is 3 times the fundamental
  528. 31:59frequency. So we just multiply the
  529. 32:03XL1 3 at times 3 anghang omega. So
  530. 32:09therefore we have now our XL3 equivalent
  531. 32:12to 56.55 55 and also the uh the
  532. 32:18capacitive reactance no so if going to
  533. 32:22change the increase
  534. 32:24the uh value of angular frequency so our
  535. 32:29inductive capacitive reactance
  536. 32:32will be will decrease no so will
  537. 32:37decrease by the multiplying factor no if
  538. 32:42we are if we are multiplying the or
  539. 32:45increasing
  540. 32:46the uh angular frequency by a factor of
  541. 32:503 our induct in our capacitive reactance
  542. 32:53will decrease by 3 or divided by 3 so
  543. 32:59therefore our xc will be equivalent to
  544. 33:028.95 95 so kung nagliog
  545. 33:07moon
  546. 33:09so that xc is 1 /
  547. 33:152π
  548. 33:17fc or omega c 1 / omega
  549. 33:22c mas dali
  550. 33:261 / omega c and if we triple this omega
  551. 33:34No so making c as our c will not change
  552. 33:38or our capacitance will not change so
  553. 33:42the value of xc will just be divided by
  554. 33:453 or if we double
  555. 33:48the so if we double the value of our
  556. 33:52angular frequency so our our xc will
  557. 33:56divided by
  558. 33:572 okay
  559. 34:00so that is how you compute for the XC on
  560. 34:06this the next
  561. 34:07harmonics. Okay.
  562. 34:10So at
  563. 34:13solbonia impedance so impedance in the
  564. 34:16third harmonic will not be and our
  565. 34:19resistance will not change
  566. 34:22ha constant no because R is not a
  567. 34:26function
  568. 34:27of any quantity. So R is the function of
  569. 34:32uh the angular frequency. No so that is
  570. 34:37why even if uh in the fifth harmony
  571. 34:40fourth harmonic so I will our R will
  572. 34:44remains the
  573. 34:46same. Okay so substitute 6 + JXL - XC so
  574. 34:526 + J 47.6 6
  575. 34:57ohms. So in the third
  576. 35:00harmonic you can see that our impedance
  577. 35:05function behaves like an RL circuit. So
  578. 35:11we already have an idea that in the
  579. 35:14third harmonic our current eye now logs
  580. 35:18the voltage by a certain angle no
  581. 35:22logging naong current danhe. So at timan
  582. 35:26ha so taking the magnitude of this
  583. 35:30quantity so you will have this
  584. 35:3248.1 ohms and solving for the RMS value
  585. 35:36of current in the third harmonic.
  586. 35:39So voltage RMS div
  587. 35:42by and that magnitude of the impedance
  588. 35:47so na siya
  589. 35:511.04. Now solving for power in the third
  590. 35:55harmonic. So we will use the third
  591. 35:59harmonic current square times the value
  592. 36:02of resistance R. So naatay 6.48.
  593. 36:0848
  594. 36:10wats the third harmonic and also we can
  595. 36:13solve now for the voltage drop across
  596. 36:16the inductor in the third
  597. 36:19harmonic so we have 58.9 9 vol and
  598. 36:26solving also for the face angle or the
  599. 36:28factor
  600. 36:29angle so we will use the power or I mean
  601. 36:34the impedence triangle
  602. 36:38so for our impedence
  603. 36:42triangle so
  604. 36:44the real part will be the r which is 6
  605. 36:49and the inductive part or the reactive
  606. 36:53part will be
  607. 36:5856
  608. 37:0055. Okay. So taking the R tangent
  609. 37:04opposite over adjacent for the XL / R.
  610. 37:09So we have this R tangent equivalent
  611. 37:13to R tangent of
  612. 37:1547.6/ 6 equ to 82.8.
  613. 37:20So what does this
  614. 37:23imply? So same as what we did in the
  615. 37:26fundamental harmonic. No. Okay. I will
  616. 37:29erase
  617. 37:34this. Okay. So as you can
  618. 37:38see our voltage no if we look back in
  619. 37:43the previous slide. So our voltage B is
  620. 37:48at 30.
  621. 37:52de socated pos
  622. 37:5830 so meaning our voltage
  623. 38:02b let us
  624. 38:06say 30°
  625. 38:09from the
  626. 38:13origin and since in the third harmonic
  627. 38:17our current eye is logging the voltage
  628. 38:20by certain angle and that angle is this
  629. 38:23angle so our eye is located somewhere
  630. 38:31here the angle between our voltage and
  631. 38:33current is
  632. 38:40828 so therefore the distance of this
  633. 38:43current I from the origin will now be
  634. 38:45equivalent to 82.8-
  635. 38:498- 30. So this is equivalent
  636. 38:53to uh
  637. 38:5982.8
  638. 39:02828 - 30 so we
  639. 39:06have 52.8.
  640. 39:11So we can express
  641. 39:14the
  642. 39:16uh current in the third harmonic no so I
  643. 39:22sub
  644. 39:253. So this will be equivalent to so RMS
  645. 39:29s of 2. So 1.04
  646. 39:3304 ro
  647. 39:362 sin
  648. 39:38of so since this is in the third
  649. 39:41harmonic o third harmonic sa na omega t
  650. 39:46and kin siya naman siya paubos no
  651. 39:52pa-counterclockwise I mean pa-clockwise
  652. 39:55clockwise direction so meaning the angle
  653. 39:57is negative so-
  654. 40:03528°. So this is your expression for
  655. 40:06current in the third harmonic. So 1.04
  656. 40:10ro 2 sin of 3 omeg t -
  657. 40:1452.8. So we have we have the last
  658. 40:18harmonic in the fifth
  659. 40:21harmonic. So fifth harmonic.
  660. 40:25So in the fifth harmonic we have the
  661. 40:26current or our voltage equivalent to
  662. 40:2928.
  663. 40:3128. I will look back. So
  664. 40:3628.28 at
  665. 40:40-2. So 28.28. So solving for the RMS. So
  666. 40:45we divide it by s of 2 and our inactive
  667. 40:49reactance will multiply by 5 no
  668. 40:54multiplied by 5 and our capacitive
  669. 40:58reactance will be divided by 5 our
  670. 41:02fundamental capacitive reactance will be
  671. 41:04divided by 5 and our
  672. 41:07fundamental uh inductive reactance will
  673. 41:11be multiplied by
  674. 41:135 So solving for the impedance in the
  675. 41:17fifth harmonic. So naay 6 + JXL which is
  676. 41:2494.25- capacitive reactance which is
  677. 41:275.37 so we have 6 + J 88.88 88 ohms. So
  678. 41:34as you can observe that impedance in the
  679. 41:37fifth harmonic behaves like an RL
  680. 41:40circuit since this is positive so RL
  681. 41:44siya then expected na that it is
  682. 41:48expected that our current in the fifth
  683. 41:50harmonic logs the voltage by a certain
  684. 41:56angle since RL circuit the R circuit
  685. 42:01ising the voltage
  686. 42:03So taking the magnitude of this quantity
  687. 42:07have this 89
  688. 42:09ohms and solving for the current in the
  689. 42:12fifth
  690. 42:13harmonic. So just substitute we have now
  691. 42:16the voltage RMS div the impedance. So
  692. 42:21you will have RMS carmonic equivalent to
  693. 42:260.225.
  694. 42:30So solving for the
  695. 42:32power. So this is equivalent to the
  696. 42:35square of the current times the
  697. 42:38resistance. So therefore you will have
  698. 42:41you have now the value for power in the
  699. 42:43harmonic equ
  700. 42:46to304
  701. 42:48watts and also the voltage drop across
  702. 42:53the inductor in the fifth
  703. 42:56harmonic you will have current times XL.
  704. 43:00This is equivalent
  705. 43:02to 2 and for the face
  706. 43:07angle so for the face angle so the same
  707. 43:11so tangent of XL over R which is
  708. 43:16equivalent to 86.1°
  709. 43:191 de okay so solving for the total RMS
  710. 43:25current or the current that our ameter
  711. 43:28will be reading this will be equivalent
  712. 43:32to the square root
  713. 43:34of the RMS in the
  714. 43:38fundamental square plus RMS value in the
  715. 43:42third harmonic plus the RMS value in the
  716. 43:46fifth harmonic so namay mga y so just
  717. 43:50substitute 10 s + 1.04 s + 20
  718. 43:550.225 square so you will have the RMS
  719. 44:00value or the total current this will be
  720. 44:03equivalent to 10.05
  721. 44:0705 and for the power so we just sum up
  722. 44:11no all the power consumed on each
  723. 44:16harmonic so the first fundamental you
  724. 44:19have 600 the third harmonic you have 648
  725. 44:236.48 48 and the third harmonic uh we
  726. 44:27have a value of
  727. 44:2934304 so in all we have total power
  728. 44:34what's consumed is
  729. 44:37606 8 and of course the total inductive
  730. 44:42voltage in the inductor so same lang
  731. 44:46kuha gap on to RMS sa VL so this will be
  732. 44:49equivalent to
  733. 44:51VRMS VLMS S in the fundamental, VLRMS in
  734. 44:56the third and VLRMS in the fifth
  735. 45:01harmonic. So ay
  736. 45:04198.8
  737. 45:06volts. Now for the equation of current
  738. 45:09wave form no at siyang-create sa una.
  739. 45:14So for the current in the first
  740. 45:16fundamental harmonic so
  741. 45:20naay
  742. 45:22pare
  743. 45:24114.14 sin omega t + 53.2 So this is the
  744. 45:29equation no equation where current in
  745. 45:32the fundamental harmonic. In the third
  746. 45:34harmonic we have this
  747. 45:371.47 sin of 3 om t -
  748. 45:4352.8. And in the third
  749. 45:45harmonic I mean in the fifth
  750. 45:47harmonic so you'll have
  751. 45:50this root of 2 * 0.25 sin of 5 om t -
  752. 45:56106.1 1 equivalent to
  753. 46:01-0.318 sin of 5 omeg t- 100.1
  754. 46:10one negative siya
  755. 46:15soat so take note that our
  756. 46:19voltage has
  757. 46:22a maximum value of negative
  758. 46:2628 and located at -
  759. 46:3220°
  760. 46:35so dinis
  761. 46:40ne 20 or
  762. 47:0020
  763. 47:02and and since
  764. 47:04our circuit in the fifth harmonic
  765. 47:08behaves like an inductive RL
  766. 47:11circuit. So logging ang kurente. So the
  767. 47:15angle between your current and voltage
  768. 47:19will be equivalent to 86.1.
  769. 47:23So somewhere
  770. 47:27here so this will be equivalent
  771. 47:31to
  772. 47:3586
  773. 47:371 so your voltage here is ne
  774. 47:4728.28 Ayan 28 no? Ano ba
  775. 47:52'to? -
  776. 47:5528.
  777. 47:5628. So if you have this voltage negative
  778. 48:00of course your current will also be
  779. 48:01negative so negative
  780. 48:04ay sub
  781. 48:065. So this angle here is
  782. 48:1186.1 and the distance of your i5 from
  783. 48:14the origin will now be equivalent to
  784. 48:1686.1
  785. 48:1920. So the expression of your current
  786. 48:22will be equivalent to this
  787. 48:27ne 2 the maximum current which is
  788. 48:330.25 sin of 5 omeg t - 106 because 86.1
  789. 48:38+ 20 is
  790. 48:40106.1 so negative si ha so - 106.1
  791. 48:45or
  792. 48:48-0.318 sin 5 om t +
  793. 48:53106.1 and therefore the complete
  794. 48:56expression for your current will now be
  795. 48:58equivalent to I1 I3 +
  796. 49:02I5 so morning naasay one
  797. 49:07ah
  798. 49:1014.4 sin of 53.12 12 +
  799. 49:14247 sin of 3 omeg t -
  800. 49:1752.8 - sin 5 om t -
  801. 49:23106.1 or we can also express this
  802. 49:28quantity in the other direction and it's
  803. 49:31opposite direction.
  804. 49:33If we going to take the opposite of this
  805. 49:35I so location will now be here. So if
  806. 49:39this is
  807. 49:40negative
  808. 49:42vector opposite vector no so this act in
  809. 49:47this direction and its opposite will be
  810. 49:49negative of
  811. 49:50this
  812. 49:52direction. Yeah. If this is 106.1
  813. 49:58And this angle now will
  814. 50:00be so an so since this is 106.1 so kay
  815. 50:0890 so 106.1-
  816. 50:1190 angle and this angle is just equal to
  817. 50:14this
  818. 50:16angle this is theta of course this angle
  819. 50:20is theta so 106.1
  820. 50:241-
  821. 50:2590 this is equivalent
  822. 50:31to 16.1 no
  823. 50:3616.1 and this is 16.1
  824. 50:40also. So 90- 16.1 so makuha so
  825. 50:4990- 16.1
  826. 50:51So have
  827. 50:5473.9
  828. 50:57[Musika]
  829. 51:0073.9
  830. 51:0273.9° so that is why we also have here
  831. 51:04another expression equivalent to and
  832. 51:07positive na ha I is positive so pos
  833. 51:120.318 318 plus ano positive
  834. 51:17+318 sin of 5 omeg t + 73.9 9 amp. So
  835. 51:22this is the complete expression for the
  836. 51:25current or you can also you can can have
  837. 51:27your answer as
  838. 51:30kanilang
  839. 51:33no pwede
  840. 51:36na
  841. 51:38kanya or pwede po kini i answer si ha.
  842. 51:44Okay. So, okay. So, so let's proceed to
  843. 51:47another
  844. 51:49example. So, this is we will now be
  845. 51:52having an example for a parallel. So,
  846. 51:55that's for series in the
  847. 51:57previous sa parallel. So, for example,
  848. 52:00given a circuit shown in figure 23 with
  849. 52:0460 cycle constant as
  850. 52:06shown 60 cycle 60 herz. So when the
  851. 52:10voltage
  852. 52:13V when the voltage V is equivalent to
  853. 52:16141.4 sin omega t + 7 sin omega t in the
  854. 52:21fundamental
  855. 52:23harmonic
  856. 52:25and in the third
  857. 52:27harmonic naatay
  858. 52:3170.7 plus 30 it's face angle is 30 and
  859. 52:34the third harmonic I mean in the fifth
  860. 52:36harmonic - 28.28 28 sin 5 om t -
  861. 52:4120 find the ameter value of the total
  862. 52:45current i
  863. 52:48so the reading of our ameter the current
  864. 52:52in each branch power dissipated by each
  865. 52:56branch total power dissipated and the
  866. 52:59equation of the resultant
  867. 53:01current so our omega or our angular
  868. 53:04frequency will be equivalent to 377 7
  869. 53:08radians per seconds. So this is our
  870. 53:12circuit no parallel branches. So RC 5
  871. 53:17ohms and 15 ohms. 5 ohms ang R C is 15.
  872. 53:22And R in the second branch connected by
  873. 53:26CD point CD. So 10 ohm resistance and 2
  874. 53:30ohms inductive reactance. Okay. So let's
  875. 53:34now solve for
  876. 53:36the um anouns nouns quantity. So as what
  877. 53:42the same as what we did on the previous
  878. 53:45example so in solving for a parallel
  879. 53:49same procedure lang. Soccerons ang iyang
  880. 53:53mga components. So for first solve for
  881. 53:56the fundamental component second in the
  882. 53:59third component or whatever component is
  883. 54:02present.
  884. 54:03And the last is the last third component
  885. 54:06or fifth fifth harmonic. Soon
  886. 54:10lang depende na kung voltage source or
  887. 54:14even current source kung upat siya na si
  888. 54:16harmonic 7 so kaupat po ka or kalima po
  889. 54:21ka mo mag-solve consider good mo kada
  890. 54:24component or kada harmonic. So first
  891. 54:27move si ka sa fundamental.
  892. 54:31So in the fundamental
  893. 54:33harmonic angipangita niya is ang current
  894. 54:37voltage sa power no total
  895. 54:42power so in the fundamental harmonic our
  896. 54:45voltage or our maximum voltage is 141.4
  897. 54:504 so divide siya 2 para makuha na to ang
  898. 54:55iyahang ah iyahang RMS value. So 100 +
  899. 55:03J0 ang voltage
  900. 55:07sa RM voltage sa fundamental. So current
  901. 55:11in the first branch can see in the first
  902. 55:19branch so to solve for the current in
  903. 55:21the first branch we need the impedance
  904. 55:23in the first branch so namay voltage
  905. 55:27100/ impedance ng 5- j15 so in the
  906. 55:30fundamental harmonic mam itong value
  907. 55:33na
  908. 55:35j15 or - j15 minus kay capacitor 1. So
  909. 55:41in the first branch we have a current
  910. 55:44of 2 + J0 or 2
  911. 55:50amp. So currents in the second
  912. 55:54branch or in the CD branch
  913. 55:58kini. So voltage divided by impedance
  914. 56:0110. So iyung quantity iyang value sa
  915. 56:03impedance is 10 + J2.
  916. 56:07So that is why
  917. 56:08100/ 10 + J2. So result niya is
  918. 56:139.62- J
  919. 56:161.925. So taking the magnitude of this
  920. 56:19current so naay
  921. 56:239.82
  922. 56:25amp. So next atong ang total in the
  923. 56:30fundamental.
  924. 56:32So total niya ang total current is
  925. 56:35just summation of the current on each
  926. 56:39branch
  927. 56:40parallel current plus current current in
  928. 56:43the fundamental harmonic. So that is
  929. 56:47IAB1
  930. 56:48plus
  931. 56:50ICD
  932. 56:521.
  933. 56:54Okay. So our current therefore will be
  934. 56:57equivalent to this quantity 12.323
  935. 57:0333.
  936. 57:06Okay. Next. Solve for the face
  937. 57:11angle. So how to solve for the face
  938. 57:14angle? So siya. So at kuha iyahang
  939. 57:19equivalent
  940. 57:21ng pwede lang gamit an current no. So
  941. 57:25real
  942. 57:29uh current the real component is
  943. 57:31equivalent to
  944. 57:3611.62 iyahang imaginary component kanina
  945. 57:40J
  946. 57:41ngang
  947. 57:454.075 so nag tangent ha r tangent of
  948. 57:494.075 / 911.62
  949. 57:5362 so naay angle equivalent to
  950. 57:5919
  951. 58:014 okay so next solve for the power in
  952. 58:05the first branch so naman tay current
  953. 58:09diha so
  954. 58:13power this will be equivalent
  955. 58:18to okay real naman eh wajer component so
  956. 58:21pwede lang anim ah the real part times
  957. 58:25the voltage so natay 200 watts and also
  958. 58:30in the second branch CD branch so 100
  959. 58:34voltage times 9.62
  960. 58:3662 real component. So pwede lang na
  961. 58:40gamitan 962 wats
  962. 58:44ng ah power in
  963. 58:48the second branch on the
  964. 58:51fundamental harmonic.
  965. 58:54Sunod and the third harmonic. So third
  966. 58:58harmonic our na our frequency or angular
  967. 59:03frequency 3 no so mahitabo ang
  968. 59:09XC maivide by 3 while our inductance or
  969. 59:15our inductive reactance XL ma-multiply
  970. 59:18by 3. So RMS value in our kuan sa volt
  971. 59:25in the third harmonic so naay 50 volts
  972. 59:30or express in kuan in rectangular
  973. 59:33coordinates of 50 + J0 imaginary
  974. 59:38component and solving for the current in
  975. 59:40the AB branch in the third harmonic soay
  976. 59:4550 volts div 5-
  977. 59:49j5 so 5 +
  978. 59:52J 5 so magnitude nga 7.07
  979. 1:00:0007 so in the CD branch 10 +
  980. 1:00:04J at 50/ 10 + J6 so
  981. 1:00:09na value 3.68 - J
  982. 1:00:152.21 in the so iang magnitude naay 4.33
  983. 1:00:20so atong i-adding du ha vector addition
  984. 1:00:23ha so 5 + 3.68 68 naay
  985. 1:00:278.68 and 5
  986. 1:00:31J5 - J2.21 so naay 2.79 so iyahang
  987. 1:00:36magnitude
  988. 1:00:399.11 so kung ano to
  989. 1:00:42i-angle so kani lang ah the imaginary
  990. 1:00:45component divided by the real component
  991. 1:00:48soay 17.85
  992. 1:00:5385 de so the same to solve for the power
  993. 1:00:58gamit real
  994. 1:01:00component 5 voltage
  995. 1:01:0550 then voltage ng 50 times sa real
  996. 1:01:08components ng current ng branch 3.68 68
  997. 1:01:14so ay
  998. 1:01:16184 watts so muna siya for the third
  999. 1:01:21harmonic next last harmonic fifth
  1000. 1:01:24harmonic so nahimong times 5 ang omega
  1001. 1:01:30no soong current or
  1002. 1:01:37voltage so
  1003. 1:01:39rms 20 or
  1004. 1:01:43orang
  1005. 1:01:45voltage equivalent to in terms of ah in
  1006. 1:01:50terms of tangular 20 +
  1007. 1:01:54j and
  1008. 1:01:56karon ayahan ng ayaahan naing kuan
  1009. 1:01:59ayahan naing xc ma-divide by 5 gikan si
  1010. 1:02:04ang fundamental ang fundamental is 15
  1011. 1:02:08man 5 so thatay Sorry ohms ah nahiya
  1012. 1:02:13hading ko an indu uh inductive inductive
  1013. 1:02:18reactance ma-multiplied by 5 so
  1014. 1:02:23naay 10 ohms so the same procedure solve
  1015. 1:02:28ka sa current in the first branch so RMS
  1016. 1:02:32voltage divided by current naatay ken
  1017. 1:02:352.94 + J.76 76
  1018. 1:02:39763 then taking its magnitude you have
  1019. 1:02:43this 3.43 amp and the next branch CD
  1020. 1:02:47branch so again 20/ 10 + J10 so ayusan
  1021. 1:02:54mo i-mine ang negative
  1022. 1:02:56haon ang k lang nagdetermin n direction
  1023. 1:03:00ha ayaw siya na i-mind only magnitude
  1024. 1:03:02sa so naatay 1- j1 or 1.414
  1025. 1:03:07414 i-add na to ang duha ka current king
  1026. 1:03:11mga current din i-add para makuha na to
  1027. 1:03:13diha in the fifth sa fifth
  1028. 1:03:15harmonic so
  1029. 1:03:17naatay current nga 3.94 +
  1030. 1:03:23j.63 or
  1031. 1:03:254.01 amp so solving for its angle tayo
  1032. 1:03:3010.95
  1033. 1:03:3395° so solving for the
  1034. 1:03:36power so voltage times the real
  1035. 1:03:39component of
  1036. 1:03:41current so 58 and 20 plus 1 only 20 wats
  1037. 1:03:49so sunod ito na kuha
  1038. 1:03:52total so the amity reading is ma ang
  1039. 1:03:55total current at point f so total
  1040. 1:03:59current is the fundamental
  1041. 1:04:0112 point or it's RMS value
  1042. 1:04:0412.33 plus the RMS value of current
  1043. 1:04:08in the third harmonic square plus the
  1044. 1:04:11third or the RMS value of current in the
  1045. 1:04:16fifth harmonics. All in all naay 15.9
  1046. 1:04:20ang maasa sa atong ameter so sa kada
  1047. 1:04:24branch sad so at
  1048. 1:04:27gamitan square root of RMS value of
  1049. 1:04:30current in the first
  1050. 1:04:32branch plus the square of the arm's
  1051. 1:04:36value of current in the second branch
  1052. 1:04:37plus the arm's value of current in the
  1053. 1:04:39third branch square. So naay 10.1 one
  1054. 1:04:42and last in the CD
  1055. 1:04:45branch mga values
  1056. 1:04:47balik so
  1057. 1:04:50value so sa first
  1058. 1:04:54branch first
  1059. 1:04:56branch first
  1060. 1:05:02branch
  1061. 1:05:10Okay. So the total power ato lang
  1062. 1:05:13ipang-sum tanan in the first branch plus
  1063. 1:05:18tan i-add na to sa second branch cd
  1064. 1:05:21branch i-add tanan. So ang total
  1065. 1:05:25niya plus power AB plus power CD have
  1066. 1:05:30this
  1067. 1:05:32quantity. Now sa current wave form
  1068. 1:05:36current wave form the fundamental
  1069. 1:05:39branch
  1070. 1:05:43so ah balik ha. So in the fundamental
  1071. 1:05:47branch so diha current kini 12.33
  1072. 1:05:5233
  1073. 1:05:54okay 12.33 33 maxim RMS na times na to
  1074. 1:05:59sa iyang s of 2 para makuha tag im in
  1075. 1:06:02the first branch or i mean in the
  1076. 1:06:04fundamental component so sin omega t +
  1077. 1:06:1019
  1078. 1:06:1244 so kung imohang kuanon kung imohang
  1079. 1:06:16solbon ang total impedance sa
  1080. 1:06:18circuit considering the
  1081. 1:06:21fundamental
  1082. 1:06:22component so diha na makita Kung un sa
  1083. 1:06:27ato ang
  1084. 1:06:27circuit it could be RL or RC. So let's
  1085. 1:06:34check para dali lang. So ato ang formula
  1086. 1:06:37na parallel
  1087. 1:06:39lang itong parallel or pwede to in terms
  1088. 1:06:42of admittance no pwede tay in terms of
  1089. 1:06:46admittance if daghan na siyang branches
  1090. 1:06:49or pwede sad
  1091. 1:06:51duhara para ato lang gamitan
  1092. 1:06:57formula sa parallel ng dua branch lang
  1093. 1:07:00du ka branches so as you can see that
  1094. 1:07:05Our
  1095. 1:07:07equivalent impedance in the fundamental
  1096. 1:07:10component is equivalent to 7.66 - J
  1097. 1:07:182.69. Okay. So un na siya so
  1098. 1:07:22RC no behaves like a capacitive branch.
  1099. 1:07:29So take note that our voltage in the
  1100. 1:07:32fundamental na lang siya sa origin
  1101. 1:07:36zero angle so siya leading
  1102. 1:07:42current so expected that our i is
  1103. 1:07:45somewhere above our
  1104. 1:07:47vle between moto nacompute ito sa i
  1105. 1:07:53194 so that is why the equation for
  1106. 1:07:56current in the fundamental branch
  1107. 1:07:59naay k r value in the
  1108. 1:08:02fundamental 2 cos of omega t plus the
  1109. 1:08:06distance sa i from the origin 19.4
  1110. 1:08:10or siya in the third
  1111. 1:08:13harmonic o same procedure so kamay
  1112. 1:08:17bahala mo na mo ah compute check lang
  1113. 1:08:22check so naay procedure ako
  1114. 1:08:25nag-introduce previously so just learn
  1115. 1:08:29from it and also in the fifth harmonic
  1116. 1:08:33ma so review mo naing siya so finally
  1117. 1:08:37equation for current
  1118. 1:08:40So you will now have the equation for
  1119. 1:08:43current equivalent
  1120. 1:08:46to ah
  1121. 1:08:4917.45
  1122. 1:08:51+ ah sin omega t + 19.4 + 12.9 sin 3
  1123. 1:08:56omeg t + 47.85 85 +
  1124. 1:09:035.67 sin 5 omeg 3 +
  1125. 1:09:08171°. Okay. So that would be all for our
  1126. 1:09:13discussion. So I hope you learn
  1127. 1:09:15something and if you are if you have any
  1128. 1:09:19question so just drop a message on
  1129. 1:09:24my social media account.
  1130. 1:09:29Okay. So that concludes our discussion
  1131. 1:09:33on the RMS value of nonsenosoidal waves.
  1132. 1:09:37So understanding how to compute and
  1133. 1:09:39interpret RMS values equip us to work
  1134. 1:09:43with real world signals.
  1135. 1:09:46system
  1136. 1:09:47efficiency and ure safety and accuracy
  1137. 1:09:51in electrical circen
  1138. 1:09:55M.

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