ProbSolv_Chapter16

ProbSolv_Chapter16 - CHAPTER 16 - FOURIER SERIES W0 List of...

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Unformatted text preview: CHAPTER 16 - FOURIER SERIES W0 List of topics for this chapter : Trigonometric Fourier Series Symmetry Considerations Circuit Applications Average Power and RMS Values Exponential Fourier Series Fourier Analysis with PSpice W6 TRIGONOMETRIC F OURIER SERIES Problem 16.1 [16.5] A voltage source has a periodic waveform defined over its period as V(t) = t(27r — t) V for 0 < t < 2n . Find the Fourier series for this voltage. 0<t<21r w0=2n/T=1 1 1 7: 1 t3 f -2 H 2-——J a0 TE (t)dt 2nf(2nt t)dt 2n rm 3 a“ 21: 3 “ 3 21tt [(Znt —- t2 ) cos(nt) dt = cos(nt) + —- sin(nt)] 3" nn n -1 an = n n3 [2nt cos(nt) — 2 sin(nt) + nth Sin(nt)] V(t) = 21tt— t2, T=21t 27: 0 -3. an—T 21: 0 1 y - 4 n n3 [4m cos(21tn)] = r17 2(1 1) a =_’ " — n n2 bn = 52: {[(Znt — t2)sin(nt) d = % I(2nt — t2)sin(nt) dt 2nl bu = —n—n—2[sin(nt)—nt005(nt)] 7mg 7‘— 0 [2m sin(nt) + 2 cos(nt) — nzt2 cos(nt)] 3" 297 Hence, 27:2 °° 4 ft =——— —cos t () 3 H; (n) Problem 16.2 Evaluate each of the following functions and determine if it is periodic. If it is periodic, find its period. (a) f(t) = cos(1tt/2) + sin(1rt) + «[3— cos(27tt) (b) y(t) = sin(\/—3_ nt)+cos(7tt) (c) g(t) = 4 + sin(mt) (d) h(t) = 25in(5t)cos(3t) (e) z(t) = e‘tsin(1tt) (a) This is a periodic function with a period of 4 seconds. (b) This is a nonperiodic function since the first term has an irrational multiplier of at while the second has a rational multiplier. (c) The integral of this function goes to infinity because of the dc function. Thus this is a nonperiodic function._ (d) This is a periodic function with a period of 7: seconds. (c) This is a nonperiodic function since it continuously changes as t goes to infinity. oma‘ SYMMETRY CONSIDERATIONS Problem 16.3 Determine the type of function represented by the signal in Figure 16.1. Also, determine the Fourier series expansion. f(t) 0 1 V V 40* V V Figure 16.1 This is an odd function since f(t) = —f(~t). Therefore, a0 = 0 = an. 298 2 T . :fj; f (t)sm(n0)ot)dt , where T = 1 sec and 030 = 2n rad/sec. 0" :1 H For 0<t<1, f(t) = 20t—10 ll Solving for bn % £(20t — 10) sin(2n7rt)dt = 2[ £20t sin(2n7tt)dt — £10 sin(2nnt)dt:l l 1 = 2 [ 220 2 sin(2n1rt) —£cos(2nnt)) —[:—1—gcos(2nnt)] 4n 11: 2m: 0 2m: 0 20 20 — 10 — 20 = 2 0—0 ~—— l—O —— 1—1 =—————— [4n2112 ( ) 2n7t( ) 2n7t( ):| 117: -—20 °° 1 , Therefore, f(t) = — —s1n(2n7tt) 7r “:1 11 Problem 16.4 [16.15] Calculate the Fourier coefficients for the function in Figure 16.2. f(t) 4 —5—4-—3—2—1 0 1 2 3 4 5 t Figure 16.2 This is an even function, therefore bn = 0. In addition, T = 4 and 030 = (0/ 2 . 2 2 a0 =¥ /2f(t) dt=Z £4tdt=t2ig =1 4 /2 4 an = :f If f (t) cos(0)0nt) dt = Z x 4t cos(n1tt/ 2) dt a) 4 2t . 1 n — 4l-n2 n2 cos(n7tt/ 2) + rm sm(n1tt/2)] 0 299 an = 2162 [cos(n7t/2)—1]+——8——sin(n7r/2) 11 1t nn Wm. CIRCUIT APPLICATIONS Problem 16.5 following values during that period, Vs(t) = 10 volts 0 < t < 1: msec = 0 nmsec<t<27r msec 100 k!) + Vs“) a E C Vout(t) Figure 16.3 In addition, L = 1 H and C = 1 uF. Determine the value of vo(t). Figure 16.3 and vs(t) is periodic with a period equal to 21: msec and has the The first step is to find the Fourier series for vs(t). an = 0 since this is an odd function. f(t) = a0 + an sin(n0)Ot) n=l T = 27mm“3 and (00 = 1000. 1 10“3 1:10'3 1 . a0 = 2n10_3 [f 10dt+ fwd Odt]= 2n10_3(10t—0)' 1 1t10"3 2 27t10‘3 ll bn f f(t)sin(1000nt)dt = 300 7:10“3 0 = 5 volts [ f")— 105in(1000t)dt + 0] 1:10~3 ~ ~~—:3-1—310 00300000 7110 x10 11 0 -_10 1th ll (cos(n7r) — 1) 22 for n = odd Thus, I bn = rm 0 for n = even °° 20 + ~—-——sin(l 000(1 + 2k)t) volts k=1 (1 + 2k)n Therefore, Vs(t) = [5 Now let us look at the first three terms. Clearly, for the dc term, Vo = 0 since the inductor looks like a short for dc. For-all the other values of n, 30 v0 = co =1000n, for n = odd 105 + L/C 1(03L —l/(coC)) j((x)L —1/(0)C)) 20L 20x106 = nth : n1: j105(0)L —1/(0)C)) + L/C j105(1000n —1000/n) +1000 (1) i For n = 1, a) = 1000. Therefore, V0 = 20/1t. For n = 3, co = 3000. Therefore, .the value olelC = —L/C— — lg)— : —j0.375§2 j(wL ~1/(03C)) — j2667 This value of impedance is so much smaller than the value of the resistor that we can neglect this term and all of the others. Thus, vo(t) = Esin(1000t) volts 1: 301 Does this answer make any sense? If we look at this term and the values of L and C, we find that L and C are in parallel resonance when a) = 1000. Thus, this circuit is actually a filter that filters out a single sine ane from the input signal. Problem 16.6 Refer to Figure 16.3. Change the value of L to (1/9) H. with everything else remaining the same. Now solve for vo(t). Everything remains the same as Problem 16.5 up till equation (a). The new value of L changes equation (a) as shown below. 20x106 . _ n 9 Thus, our new equation for V0 — 110 — — q + —— 9 n 9 For n = 1, V _ 0.7074x106 ° j105(111.11—1000) + 0.1111x106 6 E = j0.007958 — 3888.9x10 Clearly, this can be considered to be equal to zero. For n = 3, 0.235 8x106 V = 2.122 volts For all other values of n, V() is essentially equal to zero. Therefore, vo(t) = 32.m'm(3000t) = 2.122sin(3000t) v 3n Problem 16.7 [16.25] If VS in the circuit of Figure 16.4 is the same as function f2 (t) in Figure 16.5, determine the dc component and the first three nonzero harmOnics of V0 (t) . 1 Q 1 H 2 mo + vs C 1 F 1 Q V0 Figure 16.4 302 f2“) —2—1012345 t Figure 16.5 The signal is even, hence, bn = 0. In addition, T = 3 , (00 = 27t/ 3 . Vs(t)=1 fora110<t<1 Vs(t)=2 foralll<t<1.5 a0 =%[£ldt+ f5 2dtl=g . an = :1- {cos(2n1tt/3) dt + f5 2cos(2n7tt/3) dt] 3 4T 3 . 1 6 . 151 _2 . an - 3 L 21m Sln(2n7rt/3)’0 + 2m sm(2n1rt/3)ll J— rm s1n(2nn/3) 4 2 °° 1 , vS (t) = g ~ ; l~I;s1n(2n1r/3) cos(2n1tt/3) Now consider this circuit, 1 Q j2n7t/3 L, Z_[;j_3 1‘3 e _ 2m: 1—j3/2n7t _2n1t——j3 303 Z Thus: Vo Vs Simplifying, we get _ V° :12n7t+j(4n27r2—18)Vs Forthe dc case, n = 0 and Vs =3/4V and V0 = VS/2=3/8V. We can now solve for v0 (t) Vo (t) = [3+ 2A“ cos[21;nt + @n)] V n=l (6/n 7t) sin(2mt/ 3) where An = ————————-———-—— ‘/16n2 n2 + [(4n2 n2/3).- 6]2 and (9“ = 90° —— tan“ — 3 2m: where we can further simplify An to An M n7t‘l4n4 7:4 + 81 W0 AVERAGE POWER AND RMS VALUES Problem 16.8 Given the signal shown in Figure 16.6, determine the exact value of the rms V(t) 10 volts —2—10123:45 t _10I_I_II__II_ Figure 16.6 304 value of this wave shape. Using the Fourier series of the wave shape, calculate the estimated rms . value using all the terms up to and including 11 = 5. We can use the definition of VIms to calculate the rrns value of the wave shape. ’1 V,ms = —ffV2(t)dt where T = 2sec. é. fvz(t)dt=%[1:(10)2dt+ f(—10)zdt]=%[100t|; +100tIf] = 0.5[100—0+200— 100] = 100 Thus, V,ms = 100 = 10 volts. We now proceed to the Fourier series. Please note, this is just the Fourier series of a standard square wave. v(t) = ~49 lsin(n1tt), n = 2k—- 1. TC k=1n . For this problem, we want all the terms through and including 11 = 5 (k = 3). For a Fourier series, we can solve for the rms value using, Fm = /a3 +33% +bg) 1 Th v ~ errata “5’ “"5’211'37: 51: 1:2 925 = (40/1t)(0.7587) = 9.66 volts. Although this answer is only Within 5%, it is still significant enough for some cases. The reason that this is not closer to the actual value of 10 volts is that the coefficients for the Fourier series of a square wave do not decrease in value as fast as they do for other signals. 305 Problem 16.9 Given the triangular voltage wave shape shown in Figure 16.7, determine the . exact value of the rms voltage. Then, calculate the approximate value of the rms value using the Fourier terms up to and including n = 5. t 10 volts V( ) —2 —1 o 1 2 t / v 4 -10 v Figure 16.6 First we will calculate the exact value using, 1 . ,igfvzamt, where v(t) = 20t for 0<t<1/2. Note that due to symmetry, we only need to use the range, 0 < t < 1/2. Vrms 1] 1/2 0 O = (800/3)[(1/8)—0] = 100/3 800t3 1 2 _4 /2 2 _ 5fv(t)dt—§£ 400tdt— Therefore, V,ms = 10/ x/g = 5.774 volts. Now we can solve the Fourier series. The student can verify that the Fourier series for this wave shape is given by, 80 °° 1 . v(t) = —2 —2s1n(n1rt), where n = 2k— 1. 7T k=1 11 Through n = 5 we get, v(t) 5 QKSinwt) + lsin(37:t) + —1— sin(57tt) volts. 7: 9 25 Therefore, 1+ —— + —] = 5.771 volts. Clearly, this compares very favorably to the exact value of 5.774. The reason for this is because the Fourier series for a triangular wave shape converges very quickly. . 306 . Problem 16.10 [16.31] The voltage across the terminals of a circuit is v(t) = 30 + 20 cos(1201tt + 45°) + IOCos(1207tt — 45°) V The current entering the terminal at higher potential is i(t) = 6 + 4cos(1201tt + 10°) — 2003(I’120nt — 60°) A Find: (a) the rms value of the voltage, (b) the rms value of the current, (0) the average value of the power absorbed by the circuit. (a) V,ms = 1F13, +%Z(a§ +133) = 1[(30)2 43902 +102) = 33.91 V n=l —— (b) 1ms =1/62 +G)(42 + 22) = 6.782 A 1 (c) P = V... I... +~2—ZV. I. cos<®.. —<I>..) . P = (30)(60) + (0.5) [(20)(4) cos(45° —10°)— (10)(2)cos(-45° + 60°)] P = 180 + 32.76 — 9.659 = 203.1 w Problem 16.11 Determine the rms value of a triangular wave shape with a peak-to-peak value of 40 volts. If this wave shape is placed across a 10-ohm resistor, determine the average power dissipated by that resistor. As we saw in problem 16.9, the rms value of a triangular wave shape is given by, vrms = vim/‘5 = zen/3 = 11.547 volts. Average power = Vmsz/R = (11.547)2/10 = 13.333 watts. Wan—mo EXPONENTIAL FOURIER SERIES Problem 16.12 Given the sawtooth voltage wave shape shown in Figure 16.8, find its . exponential (complex) Fourier series. 307 t 10 V V0 ..—2 —1 0 1 2 t v v _r_10 v v Figure 16.7 c1] = % fv(t)e”j“‘°°'dt , where T = 1 and V(t) = (20t — 10) for 0 < t < 1. SinceT = 1,0)0 = 27:. Therefore, 0n = % £(20t - 10) e"j2"“‘dt = 20 Ite'jz’m‘dt -10 J: e'J'Z’m‘dt ~j27mt 1 te—j21mt e e —10 ~j27mt = 20 ~ "*7‘”? -_]27tn (—127tn) 0 —j21m j21m 20[ e + e 1 — j27rn O — 10 [6pm _ 21m 27m _10[_~1___J_] ' 10 21m 21m H —j2nn 47:2n2 — 41r2n2 : J— 27m ll j 1 1 20 ~——+ — [27m 41t2n2 47th2 In addition, 00 = 0. = Z _._l_1_0_ej2n7tt Thus, n=~oo m" n¢0 Problem 16.13 [16.3 7] Determine the exponential Fourier series for f (t) = t2 , -1t<t<1r,with f(t+27tn)=f(t). (no =27t/T=1 308 1 7r . c = — t2 e'J‘“ dt 0 n 27¢ Integrating by parts twice gives, 0n = 2cos(n7r/n2) = (2)(-1“/n2) , n at 0 For n=0, 1 1: 2 00:57; mtz dt=zt3— Hence, l “2 'n f(t) __+n=E— __._2_el t n¢0 W FOURIER ANALYSIS WITH PSPICE Problem 16.14 [16.51] Calculate the Fourier coefficients of the signal in Figure 16.8 using PSpice. f(t) 4 —4 ——2 0 2 4 6 8t Figure 16.8 The Schematic is shown below. In the Transient dialog box, we type “Print step = 0.01s, Final time = 36s, Center frequency = 0.1667, Output vars = v(1),” and click Enable Fourier. 309 Prob. 16.51, After simulation, the output file includes the following Fourier components, F OURIER COMPONENTS OF TRANSIENT RESPONSE V(1) DC COMPONENT = 2.000396E+00 _ HARMONIC FREQUENCY FOURIER NORMALIZED PHASE NORMALIZED (HZ) COMPONENT COMPONENT (DEG) PHASE (DEG) .- n u 310 ...
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This note was uploaded on 09/06/2010 for the course EE 50145 taught by Professor Chi during the Spring '10 term at UCSF.

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ProbSolv_Chapter16 - CHAPTER 16 - FOURIER SERIES W0 List of...

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