Matematika 3 · Stari kolokvijumi (2021/22) · rešeno i objašnjeno

Kolokvijumi — simulacije sa rešenjima

Prvi i drugi kolokvijum + oba popravna, zadatak po zadatak, sa potpunim postupkom, poenima i uputnicama na skriptu. Prvo simuliraj pod satom, pa tek onda otvaraj rešenja.

⏱️ Štoperica za simulaciju

Pravi kolokvijum traje ~90 minuta. Klikni Start pre nego što počneš — kad istekne, stani i oceni se.

Šta kolokvijumi zapravo pitaju (obrazac!)

Uporedio sam sva četiri — struktura se ponavlja gotovo identično na kolokvijumu i popravnom:

1. kolokvijum (23 poena) 2. kolokvijum (23 poena)
Zadatak 1a [5p] specijalna DJ 1. reda: Lagranžova / Rikatijeva (dato y1y_1) uslovni ekstremumi (Lagranžovi množioci) [5–6p]
Zadatak 1b [5p] LDJVR sa desnom stranom-zbirom (superpozicija, često i rezonanca) dvojni integral / zapremina [6p]
Zadatak 2a [3p] konvergencija reda: Dalamber ili Košijev koreni (uvek izađe broj ee!) krivolinijski integral 1. vrste [5–6p]
Zadatak 2b [4p] apsolutna/uslovna konvergencija alternativnog reda površinski integral 1. vrste [6p]
Zadatak 2v [6p] interval konvergencije stepenog reda (sa krajevima!) —
Šta ovo znači za tebe (potvrđeno na 9 rokova: 2018–2025!)

Kako da simuliraš kolokvijum

Recept — simulacija (radi ovo na danima 10 i 19 plana)
  1. Odštampaj ili otvori samo postavke (ne diraj rešenja!). Spremi prazan papir.
  2. Navij sat na 90 minuta. Bez skripte, bez podsetnika — kao na pravom kolokvijumu.
  3. Prvo pročitaj SVE zadatke (2 min), počni od onog čiji tip odmah prepoznaješ.
  4. Kad istekne vreme — stani. Otvori rešenja ovde i oceni se po poenima (delimičan postupak = delimični poeni).
  5. Za svaki izgubljeni poen: nađi poglavlje u skripti (uputnica je uz svaki zadatak), ponovi recept i uradi još 2 slična zadatka.

Prvi kolokvijum — 27. 4. 2022.

Zadatak 1a [5 poena]. Odrediti opšte rešenje: y=x(1+y′)+y′2\;y = x(1 + y') + y'^2  ·  Lagranžova — Skripta S1, §2.3

Prikaži rešenje

Oblik y=xf(y′)+φ(y′)y = x\,f(y') + \varphi(y') sa f(p)=1+p≠pf(p) = 1+p \neq p → Lagranžova. Smena y′=py' = p:

y=x(1+p)+p2/x′(levo dydx=p)y = x(1+p) + p^2 \;\Big/{}'_x \qquad (\text{levo } \tfrac{dy}{dx} = p)

p=1+p+(x+2p)dpdx⇒−1=(x+2p)dpdxp = 1 + p + (x + 2p)\,\frac{dp}{dx} \;\Longrightarrow\; -1 = (x+2p)\frac{dp}{dx}

Pređi na x(p)x(p) (podeli sa dpdx\frac{dp}{dx}; dxdp=x′\frac{dx}{dp} = x'):

x′=−(x+2p)⇒x′+x=−2p— linearna po x(p)x' = -(x + 2p) \;\Longrightarrow\; x' + x = -2p \quad\text{— linearna po } x(p)

Smena x=uvx = uv: iz v′+v=0v' + v = 0: v=e−pv = e^{-p}; iz u′e−p=−2pu'e^{-p} = -2p: u′=−2pepu' = -2pe^{p}, pa parcijalnom integracijom (↗ p.i.):

u=−2∫pepdp=−2ep(p−1)+cu = -2\int pe^p dp = -2e^p(p-1) + c

x=uv=ce−p−2(p−1)=ce−p−2p+2x = uv = ce^{-p} - 2(p-1) = ce^{-p} - 2p + 2

x=ce−p−2p+2,y=x(1+p)+p2x = ce^{-p} - 2p + 2, \qquad y = x(1+p) + p^2 (opšte rešenje u parametarskom obliku)

Poeni se dobijaju za: prepoznavanje tipa (1), diferenciranje + prelaz na x(p)x(p) (2), rešenu linearnu (1), zapisano parametarsko rešenje (1).

Zadatak 1b [5 poena]. Odrediti opšte rešenje: y″−4y′+8y=e2x+sin⁡2x\;y'' - 4y' + 8y = e^{2x} + \sin 2x  ·  LDJVR + superpozicija — Skripta S1, §3.2

Prikaži rešenje

Homogena: KJ r2−4r+8=0r^2 - 4r + 8 = 0: r1,2=4±16−322=2±2ir_{1,2} = \frac{4 \pm \sqrt{16-32}}{2} = 2 \pm 2i (↗ kompleksni koreni):

yh=e2x(C1cos⁡2x+C2sin⁡2x)y_h = e^{2x}(C_1\cos 2x + C_2\sin 2x)

Superpozicija — desna strana je zbir dva tipa: y=yh+yp1+yp2y = y_h + y_{p_1} + y_{p_2}.

1° Q1=e2xQ_1 = e^{2x}: a=2a = 2; koreni KJ su 2±2i≠22\pm2i \neq 2 → nije rezonanca → yp1=Ae2xy_{p_1} = Ae^{2x}:

yp1″−4yp1′+8yp1=(4A−8A+8A)e2x=4Ae2x=e2x⇒A=14y_{p_1}'' - 4y_{p_1}' + 8y_{p_1} = (4A - 8A + 8A)e^{2x} = 4Ae^{2x} = e^{2x} \;\Longrightarrow\; A = \frac14

2° Q2=sin⁡2xQ_2 = \sin 2x: α+iβ=0+2i\alpha + i\beta = 0 + 2i; nije koren KJ (2±2i2\pm2i) → yp2=Bcos⁡2x+Dsin⁡2xy_{p_2} = B\cos 2x + D\sin 2x:

yp2″=−4Bcos⁡2x−4Dsin⁡2x,yp2′=−2Bsin⁡2x+2Dcos⁡2xy_{p_2}'' = -4B\cos2x - 4D\sin2x, \qquad y_{p_2}' = -2B\sin2x + 2D\cos2x

Uvrsti i grupiši uz cos⁡2x\cos2x i sin⁡2x\sin2x:

(4B−8D)cos⁡2x+(8B+4D)sin⁡2x=sin⁡2x⇒{4B−8D=08B+4D=1⇒B=110,D=120(4B - 8D)\cos2x + (8B + 4D)\sin2x = \sin2x \;\Longrightarrow\; \begin{cases}4B - 8D = 0\\ 8B + 4D = 1\end{cases} \;\Longrightarrow\; B = \frac{1}{10},\; D = \frac{1}{20}

y=e2x(C1cos⁡2x+C2sin⁡2x)+14e2x+110cos⁡2x+120sin⁡2xy = e^{2x}(C_1\cos 2x + C_2\sin 2x) + \frac14e^{2x} + \frac{1}{10}\cos 2x + \frac{1}{20}\sin 2x

Zamka: iako Q2Q_2 ima samo sin\sin, u yp2y_{p_2} idu i cos\cos i sin\sin (i zaista B≠0B \neq 0!).

Zadatak 2a [3 poena]. Ispitati konvergenciju ∑n=1∞3nn!nn\displaystyle\sum_{n=1}^{\infty}\frac{3^nn!}{n^n}  ·  Dalamber — Skripta S1, §4.2 (identičan zadatku A.3.b sa vežbi!)

Prikaži rešenje

Faktorijel + stepeni → Dalamber:

an+1an=3n+1(n+1)!(n+1)n+1⋅nn3nn!=3(nn+1)n=3(1+1n)n→3e>1\frac{a_{n+1}}{a_n} = \frac{3^{n+1}(n+1)!}{(n+1)^{n+1}}\cdot\frac{n^n}{3^nn!} = 3\Big(\frac{n}{n+1}\Big)^n = \frac{3}{\big(1+\frac1n\big)^n} \longrightarrow \frac3e > 1

Red divergira (ℓ=3e≈1,1>1\ell = \frac3e \approx 1{,}1 > 1) — ključ: prepoznati broj ee (↗ poznati limesi).

Zadatak 2b [4 poena]. Ispitati apsolutnu i uslovnu konvergenciju ∑n=1∞(−1)nn+1−nn3\displaystyle\sum_{n=1}^{\infty}(-1)^n\frac{\sqrt{n+1}-\sqrt n}{\sqrt[3]{n}}  ·  Skripta S1, §4.3

Prikaži rešenje

Prvo sredi ana_n — racionalizacija brojioca:

n+1−n=(n+1−n)(n+1+n)n+1+n=1n+1+n⇒an=1(n+1+n)n3\sqrt{n+1}-\sqrt n = \frac{(\sqrt{n+1}-\sqrt n)(\sqrt{n+1}+\sqrt n)}{\sqrt{n+1}+\sqrt n} = \frac{1}{\sqrt{n+1}+\sqrt n} \;\Longrightarrow\; a_n = \frac{1}{(\sqrt{n+1}+\sqrt n)\sqrt[3]{n}}

Apsolutna konvergencija? Glavni deo: n+1+n∼2n\sqrt{n+1}+\sqrt n \sim 2\sqrt n, pa an∼12n1/2⋅n1/3=12n5/6a_n \sim \frac{1}{2n^{1/2}\cdot n^{1/3}} = \frac{1}{2n^{5/6}}. Drugi poredbeni sa 1n5/6\frac{1}{n^{5/6}}:

lim⁡an1/n5/6=lim⁡n5/6(n+1+n)n1/3=lim⁡n1/2n+1+n=12∈(0,∞)\lim\frac{a_n}{1/n^{5/6}} = \lim\frac{n^{5/6}}{(\sqrt{n+1}+\sqrt n)n^{1/3}} = \lim\frac{n^{1/2}}{\sqrt{n+1}+\sqrt n} = \frac12 \in (0,\infty)

∑1n5/6\sum\frac{1}{n^{5/6}} divergira (α=56≤1\alpha = \frac56 \le 1) ⇒ nije apsolutno konvergentan.

Lajbnic: an=1(n+1+n)n3a_n = \frac{1}{(\sqrt{n+1}+\sqrt n)\sqrt[3]n} — imenilac raste ⇒ (an)↓(a_n)\downarrow; i an→0a_n \to 0. ✓

Red uslovno konvergira

Zadatak 2v [6 poena]. Odrediti interval konvergencije ∑n=1∞(x−1)n(2n+1)2\displaystyle\sum_{n=1}^{\infty}\frac{(x-1)^n}{(2n+1)^2}  ·  Skripta S1, §5.1

Prikaži rešenje

Poluprečnik (Dalamber po koeficijentima):

R=lim⁡|anan+1|=lim⁡(2n+3)2(2n+1)2=1R = \lim\Big|\frac{a_n}{a_{n+1}}\Big| = \lim\frac{(2n+3)^2}{(2n+1)^2} = 1

Red konvergira za |x−1|<1|x - 1| < 1, tj. 0<x<20 < x < 2. Krajevi:

  • x=2x = 2: ∑1(2n+1)2\;\sum\frac{1}{(2n+1)^2} — poredbeni sa 1n2\frac{1}{n^2} (ℓ=14\ell = \frac14) → konvergira.
  • x=0x = 0: ∑(−1)n(2n+1)2\;\sum\frac{(-1)^n}{(2n+1)^2} — apsolutno konvergira (isti poredbeni) → konvergira.

D=[0,2]D = [0, 2] (oba kraja unutra — zato je zadatak „lak” za 6 poena: ne zaboravi krajeve!)

Popravni prvog kolokvijuma — 22. 6. 2022.

Zadatak 1a [5 poena]. y′=2cos⁡2x−sin⁡2x+y22cos⁡x\;y' = \dfrac{2\cos^2x - \sin^2x + y^2}{2\cos x}, ako je y1=asin⁡xy_1 = a\sin x partikularno rešenje  ·  Rikatijeva — Skripta S1, §2.5

Prikaži rešenje

Kvadratna po yy → Rikatijeva. Korak 1 — odredi aa: uvrsti y1=asin⁡xy_1 = a\sin x, y1′=acos⁡xy_1' = a\cos x:

acos⁡x=2cos⁡2x−sin⁡2x+a2sin⁡2x2cos⁡x/⋅2cos⁡xa\cos x = \frac{2\cos^2x - \sin^2x + a^2\sin^2x}{2\cos x} \;\Big/\cdot 2\cos x

2acos⁡2x=2cos⁡2x+(a2−1)sin⁡2x2a\cos^2x = 2\cos^2x + (a^2 - 1)\sin^2x

Da bi važilo za svako xx: uz cos⁡2x\cos^2x: 2a=2⇒a=12a = 2 \Rightarrow a = 1; uz sin⁡2x\sin^2x: a2=1a^2 = 1 ✓. Dakle y1=sin⁡xy_1 = \sin x.

Korak 2 — smena y=sin⁡x+1zy = \sin x + \frac1z, y′=cos⁡x−z′z2y' = \cos x - \frac{z'}{z^2}. Posle uvrštavanja i skraćivanja (koristi sin⁡2x+cos⁡2x=1\sin^2x + \cos^2x = 1, ↗ identiteti):

z′+ztan⁡x=−12cos⁡x— linearna po zz' + z\tan x = -\frac{1}{2\cos x} \quad\text{— linearna po } z

Korak 3 — z=uvz = uv: iz v′+vtan⁡x=0v' + v\tan x = 0: dvv=−tan⁡xdx⇒ln⁡|v|=ln⁡|cos⁡x|⇒v=cos⁡x\frac{dv}{v} = -\tan x\,dx \Rightarrow \ln|v| = \ln|\cos x| \Rightarrow v = \cos x; iz u′cos⁡x=−12cos⁡xu'\cos x = -\frac{1}{2\cos x}: u′=−12cos⁡2x⇒u=−tan⁡x2+Cu' = -\frac{1}{2\cos^2x} \Rightarrow u = -\frac{\tan x}{2} + C:

z=cos⁡x(C−tan⁡x2)=Ccos⁡x−sin⁡x2z = \cos x\Big(C - \frac{\tan x}{2}\Big) = C\cos x - \frac{\sin x}{2}

y=sin⁡x+1Ccos⁡x−sin⁡x2=sin⁡x+2C1cos⁡x−sin⁡xy = \sin x + \dfrac{1}{C\cos x - \frac{\sin x}{2}} = \sin x + \dfrac{2}{C_1\cos x - \sin x}

Provera koraka 3: z′+ztan⁡x=−Csin⁡x−cos⁡x2+Csin⁡x−sin⁡2x2cos⁡x=−cos⁡2x+sin⁡2x2cos⁡x=−12cos⁡xz' + z\tan x = -C\sin x - \frac{\cos x}{2} + C\sin x - \frac{\sin^2x}{2\cos x} = -\frac{\cos^2x + \sin^2x}{2\cos x} = -\frac{1}{2\cos x} ✓

Zadatak 1b [5 poena]. y‴−6y″+12y′−8y=1+2e2x\;y''' - 6y'' + 12y' - 8y = 1 + 2e^{2x}  ·  LDJVR: trostruki koren + rezonanca! — Skripta S1, §3.1–3.2

Prikaži rešenje

Homogena: KJ r3−6r2+12r−8=(r−2)3=0r^3 - 6r^2 + 12r - 8 = (r-2)^3 = 0 (kub binoma — zadatak 6 sa 3. vežbi!): r=2r = 2 trostruki:

yh=(C1+C2x+C3x2)e2xy_h = (C_1 + C_2x + C_3x^2)e^{2x}

Superpozicija: Q=1+2e2xQ = 1 + 2e^{2x} — dva sabirka.

1° Q1=1=e0xQ_1 = 1 = e^{0x}: a=0a = 0 nije koren KJ → yp1=Ay_{p_1} = A: uvrsti (y′=y″=y‴=0y' = y'' = y''' = 0): −8A=1⇒A=−18-8A = 1 \Rightarrow A = -\frac18.

2° Q2=2e2xQ_2 = 2e^{2x}: a=2a = 2 JESTE koren KJ višestrukosti p=3p = 3 → faktor x3x^3:

yp2=Bx3e2xy_{p_2} = Bx^3e^{2x}

Izvodi: yp2′=B(3x2+2x3)e2xy_{p_2}' = B(3x^2 + 2x^3)e^{2x}; yp2″=B(6x+12x2+4x3)e2x\;y_{p_2}'' = B(6x + 12x^2 + 4x^3)e^{2x}; yp2‴=B(6+36x+36x2+8x3)e2x\;y_{p_2}''' = B(6 + 36x + 36x^2 + 8x^3)e^{2x}.

Uvrsti — svi članovi sa xx, x2x^2, x3x^3 se potiru (provera: uz xx: 36−36=036 - 36 = 0; uz x2x^2: 36−72+36=036 - 72 + 36 = 0; uz x3x^3: 8−24+24−8=08 - 24 + 24 - 8 = 0):

6Be2x=2e2x⇒B=136Be^{2x} = 2e^{2x} \;\Longrightarrow\; B = \frac13

y=(C1+C2x+C3x2)e2x−18+x33e2xy = (C_1 + C_2x + C_3x^2)e^{2x} - \frac18 + \frac{x^3}{3}e^{2x}

Ovo je NAJTEŽA rezonanca koja se pojavila: aa = trostruki koren → x3x^3. Ako zaboraviš faktor — sve se poništi i nema rešenja.

Zadatak 2a [3 poena]. Ispitati konvergenciju ∑n=1∞3n(nn+1)n2\displaystyle\sum_{n=1}^{\infty}3^n\Big(\frac{n}{n+1}\Big)^{n^2}  ·  Košijev koreni — Skripta S1, §4.2

Prikaži rešenje

Stepen n2n^2 → koreni kriterijum:

ann=3(nn+1)n=3(1+1n)n→3e>1\sqrt[n]{a_n} = 3\Big(\frac{n}{n+1}\Big)^n = \frac{3}{\big(1+\frac1n\big)^n} \longrightarrow \frac3e > 1

Red divergira (isti limes 3e\frac3e kao na redovnom roku — samo Koši umesto Dalambera!)

Zadatak 2b [4 poena]. Apsolutna i uslovna konvergencija ∑n=1∞(−1)nln⁡(n+1)\displaystyle\sum_{n=1}^{\infty}\frac{(-1)^n}{\ln(n+1)}  ·  identičan zadatku B.1.b sa 4. vežbi!

Prikaži rešenje

Apsolutna? ln⁡(n+1)<n+1⇒1ln⁡(n+1)>1n+1\ln(n+1) < n+1 \Rightarrow \frac{1}{\ln(n+1)} > \frac{1}{n+1}, a ∑1n+1\sum\frac{1}{n+1} divergira → po 1. poredbenom ∑1ln⁡(n+1)\sum\frac{1}{\ln(n+1)} divergira ⇒ nije apsolutna.

Lajbnic: ln\ln raste ⇒ an=1ln⁡(n+1)↓a_n = \frac{1}{\ln(n+1)}\downarrow; an→0\;a_n \to 0 ✓.

Red uslovno konvergira

Zadatak 2v [6 poena]. Interval konvergencije ∑n=1∞(x+2)nn(n+1)(n+2)\displaystyle\sum_{n=1}^{\infty}\frac{(x+2)^n}{n(n+1)(n+2)}

Prikaži rešenje

Poluprečnik:

R=lim⁡|anan+1|=lim⁡(n+1)(n+2)(n+3)n(n+1)(n+2)=lim⁡n+3n=1R = \lim\Big|\frac{a_n}{a_{n+1}}\Big| = \lim\frac{(n+1)(n+2)(n+3)}{n(n+1)(n+2)} = \lim\frac{n+3}{n} = 1

Konvergira za |x+2|<1|x+2| < 1, tj. −3<x<−1-3 < x < -1. Krajevi:

  • x=−1x = -1: ∑1n(n+1)(n+2)\;\sum\frac{1}{n(n+1)(n+2)} — poredbeni sa 1n3\frac{1}{n^3} → konvergira.
  • x=−3x = -3: ∑(−1)nn(n+1)(n+2)\;\sum\frac{(-1)^n}{n(n+1)(n+2)} — apsolutno konvergira → konvergira.

D=[−3,−1]D = [-3, -1]

Drugi kolokvijum — 12. 6. 2022.

Zadatak 1 [6 poena]. Odrediti uslovne ekstremume f(x,y,z)=x−2y+2zf(x,y,z) = x - 2y + 2z uz x2+y2+z2=1x^2+y^2+z^2 = 1  ·  Lagranž — Skripta S2, §7.3

Prikaži rešenje

F=x−2y+2z+λ(x2+y2+z2−1)F = x - 2y + 2z + \lambda(x^2+y^2+z^2-1)

Fx=1+2λx=0,Fy=−2+2λy=0,Fz=2+2λz=0⇒x=−12λ,y=1λ,z=−1λF_x = 1 + 2\lambda x = 0, \quad F_y = -2 + 2\lambda y = 0, \quad F_z = 2 + 2\lambda z = 0 \;\Longrightarrow\; x = -\frac{1}{2\lambda},\; y = \frac1\lambda,\; z = -\frac1\lambda

Uvrsti u uslov:

14λ2+1λ2+1λ2=1⇒94λ2=1⇒λ=±32\frac{1}{4\lambda^2} + \frac{1}{\lambda^2} + \frac{1}{\lambda^2} = 1 \;\Longrightarrow\; \frac{9}{4\lambda^2} = 1 \;\Longrightarrow\; \lambda = \pm\frac32

  • λ=32\lambda = \frac32: M1(−13,23,−23)M_1\big({-\frac13}, \frac23, {-\frac23}\big); d2F=2λ((dx)2+(dy)2+(dz)2)>0\;d^2F = 2\lambda\big((dx)^2+(dy)^2+(dz)^2\big) > 0 → uslovni minimum, f(M1)=−13−43−43=−3f(M_1) = -\frac13 - \frac43 - \frac43 = -3.
  • λ=−32\lambda = -\frac32: M2(13,−23,23)M_2\big(\frac13, {-\frac23}, \frac23\big); d2F<0\;d^2F < 0 → uslovni maksimum, f(M2)=3f(M_2) = 3.

fmin=−3f_{\min} = -3 u M1M_1; fmax=3\;f_{\max} = 3 u M2M_2

Brza kontrola: linearna funkcija na jediničnoj sferi ima ekstreme ±∥(1,−2,2)∥=±1+4+4=±3\pm\|(1,-2,2)\| = \pm\sqrt{1+4+4} = \pm3 ✓

Zadatak 2 [6 poena]. Izračunati ∬D2ydxdy\displaystyle\iint_D 2y\,dxdy, gde je DD ograničena pravama y=xy = x, y=x+1y = x+1, x=0x = 0, x=2x = 2  ·  dvojni integral — Skripta S2, §8.1

Prikaži rešenje

Oblast je „kosa traka” između dve paralelne prave, odsečena vertikalama — projekcija na xx-osu daje jedan komad:

D={0≤x≤2,x≤y≤x+1}D = \{0 \le x \le 2,\; x \le y \le x+1\}

∬D2ydxdy=∫02dx∫xx+12ydy=∫02y2|xx+1dx=∫02((x+1)2−x2)dx=∫02(2x+1)dx\iint_D 2y\,dxdy = \int_0^2 dx\int_x^{x+1}2y\,dy = \int_0^2 y^2\Big|_x^{x+1}dx = \int_0^2\big((x+1)^2 - x^2\big)dx = \int_0^2(2x+1)\,dx

=(x2+x)|02=4+2=<span class="rezultat">6</span>= \big(x^2 + x\big)\Big|_0^2 = 4 + 2 = \text{<span class="rezultat">$6$</span>}

Poenta zadatka: pravilno opisati oblast (skiciraj!); sam račun je kratak.

Zadatak 3 [5 poena]. Izračunati I=∫C(x2+y2+z2)dsI = \displaystyle\int_C(x^2+y^2+z^2)\,ds, gde je CC: x=2cos⁡tx = 2\cos t, y=2sin⁡ty = 2\sin t, z=3tz = 3t, t∈[0,2π]t\in[0,2\pi]  ·  krivolinijski 1. vrste (heliks) — Skripta S2, §9.1

Prikaži rešenje

Integrand na krivoj: x2+y2=4cos⁡2t+4sin⁡2t=4x^2 + y^2 = 4\cos^2t + 4\sin^2t = 4; z2=9t2\;z^2 = 9t^2 → integrand =4+9t2= 4 + 9t^2.

Element luka: x′=−2sin⁡tx' = -2\sin t, y′=2cos⁡ty' = 2\cos t, z′=3z' = 3:

ds=4sin⁡2t+4cos⁡2t+9dt=13dtds = \sqrt{4\sin^2t + 4\cos^2t + 9}\,dt = \sqrt{13}\,dt

I=13∫02π(4+9t2)dt=13(4t+3t3)|02π=13(8π+24π3)I = \sqrt{13}\int_0^{2\pi}(4 + 9t^2)\,dt = \sqrt{13}\Big(4t + 3t^3\Big)\Big|_0^{2\pi} = \sqrt{13}\,\big(8\pi + 24\pi^3\big)

I=813π(1+3π2)I = 8\sqrt{13}\,\pi\big(1 + 3\pi^2\big)

Tipično za heliks: dsds je konstanta — sva „težina” zadatka je u urednom integraljenju po tt.

Zadatak 4 [6 poena]. Izračunati ∬Sx2z2dS\displaystyle\iint_S x^2z^2\,dS, gde je SS deo konusa z=x2+y2z = \sqrt{x^2+y^2} između ravni z=az = a i z=bz = b (0<a<b0 < a < b)  ·  površinski 1. vrste — Skripta S2, §9.3

Prikaži rešenje

Element površi za konus: p=xx2+y2p = \frac{x}{\sqrt{x^2+y^2}}, q=yx2+y2q = \frac{y}{\sqrt{x^2+y^2}}, pa 1+p2+q2=2\sqrt{1+p^2+q^2} = \sqrt2 (uvek za ovaj konus!):

dS=2dxdydS = \sqrt2\,dxdy

Projekcija: a≤z=x2+y2≤ba \le z = \sqrt{x^2+y^2} \le b ⇒ prsten a2≤x2+y2≤b2a^2 \le x^2+y^2 \le b^2.

Integrand: z2=x2+y2z^2 = x^2+y^2, pa x2z2=x2(x2+y2)x^2z^2 = x^2(x^2+y^2). Polarne koordinate: x2=ρ2cos⁡2φx^2 = \rho^2\cos^2\varphi:

I=2∬prstenx2(x2+y2)dxdy=2∫02πcos⁡2φdφ∫abρ4⋅ρdρI = \sqrt2\iint_{\text{prsten}}x^2(x^2+y^2)\,dxdy = \sqrt2\int_0^{2\pi}\cos^2\varphi\,d\varphi\int_a^b\rho^4\cdot\rho\,d\rho

=2⋅π⋅ρ66|ab(∫02πcos⁡2φdφ=π,<a class="cs" href="cheatsheet.html#trig-identiteti">↗ identiteti</a>)= \sqrt2\cdot\pi\cdot\frac{\rho^6}{6}\Big|_a^b \qquad\Big(\int_0^{2\pi}\cos^2\varphi\,d\varphi = \pi,\; \text{<a class="cs" href="cheatsheet.html#trig-identiteti">↗ identiteti</a>}\Big)

I=2π(b6−a6)6I = \dfrac{\sqrt2\,\pi\,(b^6 - a^6)}{6}

Popravni drugog kolokvijuma — 22. 6. 2022.

Zadatak 1 [5 poena]. Uslovni ekstremumi f(x,y)=x2+xy+y2f(x,y) = x^2 + xy + y^2 uz x2+y2=1x^2 + y^2 = 1  ·  Lagranž — Skripta S2, §7.3

Prikaži rešenje

F=x2+xy+y2+λ(x2+y2−1):Fx=(2+2λ)x+y=0,Fy=x+(2+2λ)y=0F = x^2 + xy + y^2 + \lambda(x^2+y^2-1): \qquad F_x = (2+2\lambda)x + y = 0, \quad F_y = x + (2+2\lambda)y = 0

Homogen sistem ima netrivijalno rešenje kad je determinanta nula:

(2+2λ)2−1=0⇒2+2λ=±1⇒λ=−12iliλ=−32(2+2\lambda)^2 - 1 = 0 \;\Longrightarrow\; 2+2\lambda = \pm1 \;\Longrightarrow\; \lambda = -\frac12 \;\text{ili}\; \lambda = -\frac32

λ=−12\lambda = -\frac12: iz x+y=0x + y = 0: y=−xy = -x; uslov 2x2=12x^2 = 1: tačke (±22,∓22)\big({\pm\frac{\sqrt2}{2}}, {\mp\frac{\sqrt2}{2}}\big). Vrednost: f=x2+y2⏟=1+xy=1−12=12f = \underbrace{x^2+y^2}_{=1} + xy = 1 - \frac12 = \frac12.

λ=−32\lambda = -\frac32: iz −x+y=0-x + y = 0: y=xy = x; tačke (±22,±22)\big({\pm\frac{\sqrt2}{2}}, {\pm\frac{\sqrt2}{2}}\big). Vrednost: f=1+12=32f = 1 + \frac12 = \frac32.

Klasifikacija (d2F=(2+2λ)((dx)2+(dy)2)+2dxdyd^2F = (2+2\lambda)\big((dx)^2+(dy)^2\big) + 2\,dx\,dy, uz diferenciranu vezu xdx+ydy=0x\,dx + y\,dy = 0):

  • λ=−12\lambda = -\frac12: d2F=(dx+dy)2d^2F = (dx+dy)^2; veza u (22,−22)\big(\frac{\sqrt2}{2}, -\frac{\sqrt2}{2}\big) daje dx=dydx = dy, pa d2F=4(dx)2>0d^2F = 4(dx)^2 > 0 → uslovni minimum, f=12f = \frac12.
  • λ=−32\lambda = -\frac32: d2F=−(dx−dy)2d^2F = -(dx-dy)^2; veza u (22,22)\big(\frac{\sqrt2}{2}, \frac{\sqrt2}{2}\big) daje dy=−dxdy = -dx, pa d2F=−4(dx)2<0d^2F = -4(dx)^2 < 0 → uslovni maksimum, f=32f = \frac32.

fmin=12f_{\min} = \frac12 u (±22,∓22)\big({\pm\frac{\sqrt2}{2}}, {\mp\frac{\sqrt2}{2}}\big); fmax=32\;f_{\max} = \frac32 u (±22,±22)\big({\pm\frac{\sqrt2}{2}}, {\pm\frac{\sqrt2}{2}}\big)

Zamka: d2Fd^2F je ovde semi-definitan sam po sebi — mora se uvrstiti diferencirana veza (korak koji nosi poene!).

Zadatak 2 [6 poena]. Izračunati zapreminu oblasti VV ograničene paraboloidom z=2+x2+y2z = 2 + x^2 + y^2 i ravni z=6z = 6, pri čemu je y≥0y \ge 0  ·  zapremina — Skripta S2, §8.2

Prikaži rešenje

Presek: 2+x2+y2=6⇒x2+y2=42 + x^2 + y^2 = 6 \Rightarrow x^2 + y^2 = 4. Zbog y≥0y \ge 0 projekcija je polukrug poluprečnika 2.

V=∬D(6−(2+x2+y2))dxdy=∬D(4−(x2+y2))dxdyV = \iint_{D}\big(6 - (2 + x^2 + y^2)\big)\,dxdy = \iint_D\big(4 - (x^2+y^2)\big)\,dxdy

Polarne koordinate — polukrug znači φ∈[0,π]\varphi \in [0, \pi] (ne 2π2\pi!):

V=∫0πdφ∫02(4−ρ2)ρdρ=π(2ρ2−ρ44)|02=π(8−4)V = \int_0^{\pi}d\varphi\int_0^2(4-\rho^2)\,\rho\,d\rho = \pi\Big(2\rho^2 - \frac{\rho^4}{4}\Big)\Big|_0^2 = \pi(8 - 4)

V=4πV = 4\pi

Zamka: uslov y≥0y \ge 0 prepolovljava telo — ceo krug bi dao 8π8\pi.

Zadatak 3 [6 poena]. Izračunati I=∮C(x+y)dsI = \displaystyle\oint_C(x+y)\,ds, gde je CC granica trougla O(0,0)O(0,0), A(1,0)A(1,0), B(0,1)B(0,1)  ·  identičan zadatku 2 sa 9. vežbi!

Prikaži rešenje

Tri stranice (orijentacija nebitna za 1. vrstu):

  • OA¯\overline{OA}: y=0y = 0, ds=dxds = dx: ∫01xdx=12\;\int_0^1x\,dx = \frac12
  • AB¯\overline{AB}: y=1−xy = 1-x, y′=−1y' = -1, ds=2dxds = \sqrt2\,dx; integrand x+(1−x)=1x + (1-x) = 1: 2∫01dx=2\;\sqrt2\int_0^1dx = \sqrt2
  • BO¯\overline{BO}: x=0x = 0, ds=dyds = dy: ∫01ydy=12\;\int_0^1y\,dy = \frac12

I=12+2+12=1+2I = \frac12 + \sqrt2 + \frac12 = 1 + \sqrt2

Zadatak 4 [6 poena]. Izračunati I=∬S(6x+4y+3z)dSI = \displaystyle\iint_S(6x + 4y + 3z)\,dS, gde je SS deo ravni x+2y+3z=6x + 2y + 3z = 6 za x,y,z≥0x, y, z \ge 0  ·  površinski 1. vrste — Skripta S2, §9.3

Prikaži rešenje

Površ: z=6−x−2y3=2−x3−2y3z = \frac{6 - x - 2y}{3} = 2 - \frac x3 - \frac{2y}{3}: p=−13\;p = -\frac13, q=−23q = -\frac23:

dS=1+19+49dxdy=149dxdy=143dxdydS = \sqrt{1 + \frac19 + \frac49}\,dxdy = \sqrt{\frac{14}{9}}\,dxdy = \frac{\sqrt{14}}{3}\,dxdy

Integrand na ravni — uprosti pre integraljenja (trik!): 3z=6−x−2y3z = 6 - x - 2y, pa

6x+4y+3z=6x+4y+6−x−2y=5x+2y+66x + 4y + 3z = 6x + 4y + 6 - x - 2y = 5x + 2y + 6

Projekcija (z≥0⇒x+2y≤6z \ge 0 \Rightarrow x + 2y \le 6; x,y≥0x, y \ge 0): trougao sa temenima (0,0)(0,0), (6,0)(6,0), (0,3)(0,3): D={0≤x≤6,0≤y≤6−x2}\;D = \{0 \le x \le 6,\; 0 \le y \le \frac{6-x}{2}\}.

∬D(5x+2y+6)dxdy=∫06(5xy+y2+6y)|06−x2dx=∫06(5x(6−x)2+(6−x)24+3(6−x))dx\iint_D(5x + 2y + 6)\,dxdy = \int_0^6\Big(5xy + y^2 + 6y\Big)\Big|_0^{\frac{6-x}{2}}dx = \int_0^6\Big(\frac{5x(6-x)}{2} + \frac{(6-x)^2}{4} + 3(6-x)\Big)dx

Tri dela: 52∫06(6x−x2)dx=52⋅36=90\;\frac52\int_0^6(6x - x^2)dx = \frac52\cdot36 = 90; 14∫06(6−x)2dx=14⋅2163=18\;\frac14\int_0^6(6-x)^2dx = \frac14\cdot\frac{216}{3} = 18; 3∫06(6−x)dx=3⋅18=54\;3\int_0^6(6-x)dx = 3\cdot18 = 54. Zbir: 162162.

I=143⋅162I = \frac{\sqrt{14}}{3}\cdot162

I=5414I = 54\sqrt{14}

Prvi kolokvijum — 26. 4. 2023.

Zadatak 1a [5 poena]. y′2+(x−2)y′−y+1=0\;y'^2 + (x-2)y' - y + 1 = 0  ·  prerušena Klerova!

Prikaži rešenje

Trik: izrazi yy i grupiši uz xx:

y=y′2+(x−2)y′+1=xy′+(y′2−2y′+1)=xy′+(y′−1)2y = y'^2 + (x-2)y' + 1 = xy' + \big(y'^2 - 2y' + 1\big) = xy' + (y'-1)^2

— Klerova sa φ(p)=(p−1)2\varphi(p) = (p-1)^2!

Opšte (y′→Cy' \to C): y=Cx+(C−1)2y = Cx + (C-1)^2

Singularno: x=−φ′(p)=−2(p−1)⇒p=1−x2x = -\varphi'(p) = -2(p-1) \Rightarrow p = 1 - \frac x2; y=xp+(p−1)2=x(1−x2)+x24\;y = xp + (p-1)^2 = x\big(1-\frac x2\big) + \frac{x^2}{4}:

y=x−x24y = x - \dfrac{x^2}{4} (provera uvrštavanjem: ✓)

Zadatak 1b [5 poena]. y″−2y′+y=4ex+2sin⁡x\;y'' - 2y' + y = 4e^x + 2\sin x  ·  dvostruki koren + rezonanca sa x2x^2!

Prikaži rešenje

Homogena: KJ (r−1)2=0⇒r=1(r-1)^2 = 0 \Rightarrow r = 1 dvostruki: yh=(C1+C2x)exy_h = (C_1 + C_2x)e^x.

1° Q1=4exQ_1 = 4e^x: a=1a = 1 je koren višestrukosti 2 → faktor x2x^2: yp1=Ax2exy_{p_1} = Ax^2e^x.

Uvrsti (yp1″=A(2+4x+x2)exy_{p_1}'' = A(2 + 4x + x^2)e^x, yp1′=A(2x+x2)exy_{p_1}' = A(2x+x^2)e^x):

Aex[(2+4x+x2)−2(2x+x2)+x2]=2Aex=4ex⇒A=2A e^x\big[(2+4x+x^2) - 2(2x+x^2) + x^2\big] = 2Ae^x = 4e^x \;\Longrightarrow\; A = 2

2° Q2=2sin⁡xQ_2 = 2\sin x: ii nije koren → yp2=Bcos⁡x+Dsin⁡xy_{p_2} = B\cos x + D\sin x; uvrštavanjem: uz cos\cos: −2D=0-2D = 0… pažljivo:

(−Bcos⁡−Dsin⁡)−2(−Bsin⁡+Dcos⁡)+(Bcos⁡+Dsin⁡)=−2Dcos⁡x+2Bsin⁡x=2sin⁡x(-B\cos - D\sin) - 2(-B\sin + D\cos) + (B\cos + D\sin) = -2D\cos x + 2B\sin x = 2\sin x

D=0D = 0, B=1B = 1: yp2=cos⁡xy_{p_2} = \cos x.

y=(C1+C2x)ex+2x2ex+cos⁡xy = (C_1 + C_2x)e^x + 2x^2e^x + \cos x

Zadatak 2a [5 poena]. Konvergencija ∑n=2∞1nln⁡2n\displaystyle\sum_{n=2}^{\infty}\frac{1}{n\ln^2 n}  ·  identičan zadatku A.5 sa vežbi!

Prikaži rešenje

Integralni kriterijum, smena t=ln⁡xt = \ln x: ∫2∞dxxln⁡2x=∫ln⁡2∞dtt2=1ln⁡2<∞\;\int_2^{\infty}\frac{dx}{x\ln^2x} = \int_{\ln2}^{\infty}\frac{dt}{t^2} = \frac{1}{\ln 2} < \infty.

Red konvergira

Zadatak 2b [4 poena]. Apsolutna/uslovna konvergencija ∑n=1∞(−1)n+12n+1n(n+1)\displaystyle\sum_{n=1}^{\infty}(-1)^{n+1}\frac{2n+1}{n(n+1)}  ·  identičan zadatku B.1.a sa vežbi!

Prikaži rešenje

Apsolutni red ∼2n\sim \frac2n (2. poredbeni sa 1n\frac1n, ℓ=2\ell = 2) → divergira. Lajbnic: an+1−an=−2n(n+2)<0a_{n+1} - a_n = -\frac{2}{n(n+2)} < 0 i an→0a_n\to0 ✓.

Uslovno konvergira

Zadatak 2v [4 poena]. Interval konvergencije ∑n=1∞(−1)nx2n(2n)!\displaystyle\sum_{n=1}^{\infty}(-1)^n\frac{x^{2n}}{(2n)!}  ·  pazi: stepeni x2nx^{2n}!

Prikaži rešenje

Zbog x2nx^{2n} radi direktno Dalamberom na ceo član:

lim⁡|x2n+2/(2n+2)!x2n/(2n)!|=lim⁡x2(2n+1)(2n+2)=0<1za svako x\lim\Big|\frac{x^{2n+2}/(2n+2)!}{x^{2n}/(2n)!}\Big| = \lim\frac{x^2}{(2n+1)(2n+2)} = 0 < 1 \quad\text{za svako } x

D=(−∞,+∞)=ℝD = (-\infty, +\infty) = \mathbb{R} (ovo je red za cos⁡x−1\cos x - 1 — konvergira svuda!)

Drugi kolokvijum — 6. 6. 2023.

Zadatak 1 [6 poena]. Uslovni ekstremumi f(x,y)=6−4x−3yf(x,y) = 6 - 4x - 3y uz x2+y2=1x^2+y^2 = 1

Prikaži rešenje

F=6−4x−3y+λ(x2+y2−1)F = 6 - 4x - 3y + \lambda(x^2+y^2-1): iz Fx=−4+2λx=0F_x = -4 + 2\lambda x = 0, Fy=−3+2λy=0F_y = -3 + 2\lambda y = 0: x=2λx = \frac{2}{\lambda}, y=32λy = \frac{3}{2\lambda}.

Uslov: 4λ2+94λ2=1⇒254λ2=1⇒λ=±52\frac{4}{\lambda^2} + \frac{9}{4\lambda^2} = 1 \Rightarrow \frac{25}{4\lambda^2} = 1 \Rightarrow \lambda = \pm\frac52.

  • λ=52\lambda = \frac52: M1(45,35)M_1\big(\frac45, \frac35\big), d2F=2λ(…)>0d^2F = 2\lambda(\ldots) > 0 → min, f=6−165−95=1f = 6 - \frac{16}{5} - \frac95 = 1.
  • λ=−52\lambda = -\frac52: M2(−45,−35)M_2\big({-\frac45}, {-\frac35}\big) → max, f=11f = 11.

fmin=1f_{\min} = 1, fmax=11f_{\max} = 11 (kontrola: 6∓∥(−4,−3)∥=6∓56 \mp \|(-4,-3)\| = 6\mp5 ✓)

Zadatak 2 [6 poena]. ∬Dxy2dxdy\displaystyle\iint_D xy^2\,dxdy; DD između parabole y2=2xy^2 = 2x i prave x=12x = \frac12

Prikaži rešenje

Presek: y2=1⇒y=±1y^2 = 1 \Rightarrow y = \pm1. Projekcija na yy-osu (parabola sleva? ne — parabola je leva granica x=y22x = \frac{y^2}{2}, prava desna):

D={−1≤y≤1,y22≤x≤12}D = \Big\{{-1} \le y \le 1,\; \frac{y^2}{2} \le x \le \frac12\Big\}

∬=∫−11y2dy∫y2/21/2xdx=∫−11y2⋅x22|y2/21/2dy=18∫−11(y2−y6)dy=18⋅2(13−17)=14⋅421\iint = \int_{-1}^1 y^2\,dy\int_{y^2/2}^{1/2}x\,dx = \int_{-1}^1y^2\cdot\frac{x^2}{2}\Big|_{y^2/2}^{1/2}dy = \frac18\int_{-1}^1\big(y^2 - y^6\big)dy = \frac18\cdot2\Big(\frac13 - \frac17\Big) = \frac14\cdot\frac{4}{21}

121\dfrac{1}{21} (parnost: 2∫012\int_0^1!)

Zadatak 3 [5 poena]. I=∫C(x−2y2)dsI = \displaystyle\int_C(x - 2y^2)\,ds; CC: deo prave y=−1−xy = -1-x od A(−1,0)A(-1,0) do B(0,−1)B(0,-1)

Prikaži rešenje

Parametrizacija: x=tx = t, y=−1−ty = -1-t, t∈[−1,0]t\in[-1, 0]; y′=−1⇒ds=2dty' = -1 \Rightarrow ds = \sqrt2\,dt.

I=2∫−10(t−2(1+t)2)dt=2[t22|−10⋅…]=2(−12−23)I = \sqrt2\int_{-1}^0\big(t - 2(1+t)^2\big)dt = \sqrt2\Big[\frac{t^2}{2}\Big|_{-1}^0\cdot\ldots\Big] = \sqrt2\Big({-\frac12} - \frac23\Big)

(∫−10tdt=−12\int_{-1}^0t\,dt = -\frac12; ∫−102(1+t)2dt=23(1+t)3|−10⋅…=23\int_{-1}^0 2(1+t)^2dt = \frac23(1+t)^3\big|_{-1}^0\cdot\ldots = \frac23)

I=−726I = -\dfrac{7\sqrt2}{6} (može biti negativan — integrand menja znak, ds>0ds > 0!)

Zadatak 4 [6 poena]. ∬Sy(x+z2)dS\displaystyle\iint_S y(x+z^2)\,dS; SS: deo konusa z=−x2+y2z = -\sqrt{x^2+y^2} unutar cilindra x2+y2=2yx^2+y^2 = 2y

Prikaži rešenje

Donji konus — ali dSdS je isti: p=−xx2+y2p = \frac{-x}{\sqrt{x^2+y^2}}, q=−yx2+y2q = \frac{-y}{\sqrt{x^2+y^2}}, 1+p2+q2=2\sqrt{1+p^2+q^2} = \sqrt2, i z2=x2+y2z^2 = x^2+y^2.

Projekcija: x2+y2≤2y⇔x2+(y−1)2≤1x^2+y^2 \le 2y \iff x^2 + (y-1)^2 \le 1 — krug centra (0,1)(0,1); u polarnim ρ≤2sin⁡φ\rho \le 2\sin\varphi, φ∈[0,π]\varphi\in[0,\pi].

I=2∬Dy(x+x2+y2)dxdy=2[∬Dxy⏟=0(simetrija po x)+∬Dy(x2+y2)]I = \sqrt2\iint_D y\big(x + x^2+y^2\big)dxdy = \sqrt2\Big[\underbrace{\iint_D xy}_{=0\ \text{(simetrija po }x)} + \iint_D y(x^2+y^2)\Big]

∬Dy(x2+y2)=∫0π∫02sin⁡φρsin⁡φ⋅ρ2⋅ρdρdφ=∫0πsin⁡φ⋅(2sin⁡φ)44...wait—dφ=4∫0πsin⁡5φdφ=4⋅1615\iint_D y(x^2+y^2) = \int_0^{\pi}\!\!\int_0^{2\sin\varphi}\rho\sin\varphi\cdot\rho^2\cdot\rho\,d\rho\,d\varphi = \int_0^{\pi}\sin\varphi\cdot\frac{(2\sin\varphi)^4}{4}\,... wait — d\varphi = 4\int_0^{\pi}\sin^5\varphi\,d\varphi = 4\cdot\frac{16}{15}

(∫0πsin⁡5=2⋅815\int_0^{\pi}\sin^5 = 2\cdot\frac{8}{15} — Valisove formule)

I=64215I = \dfrac{64\sqrt2}{15}

Rok 22. 10. 2025. — oba dela (najnoviji format!)

Prvi deo

Zadatak 1a [5 poena]. Odrediti opšte i singularno rešenje: y=xy′−(y′)33\;y = xy' - \dfrac{(y')^3}{3}

Prikaži rešenje

Klerova sa φ(p)=−p33\varphi(p) = -\frac{p^3}{3}.

Opšte: y=Cx−C33y = Cx - \dfrac{C^3}{3}

Singularno: x=−φ′(p)=p2x = -\varphi'(p) = p^2; y=xp−p33=p3−p33=2p33\;y = xp - \frac{p^3}{3} = p^3 - \frac{p^3}{3} = \frac{2p^3}{3}. Eliminacija (p=±xp = \pm\sqrt x):

y=±23x3/2y = \pm\dfrac23x^{3/2}, tj. 9y2=4x39y^2 = 4x^3 (provera za y=23x3/2y = \frac23x^{3/2}: y′=xy' = \sqrt x, xy′−x3/23=23x3/2xy' - \frac{x^{3/2}}{3} = \frac23x^{3/2} ✓)

Zadatak 1b [5 poena]. y″−2y′−3y=25x2e4x\;y'' - 2y' - 3y = 25x^2e^{4x}

Prikaži rešenje

KJ: r2−2r−3=(r−3)(r+1)=0r^2 - 2r - 3 = (r-3)(r+1) = 0: yh=C1e3x+C2e−xy_h = C_1e^{3x} + C_2e^{-x}.

a=4a = 4 nije koren → yp=(Ax2+Bx+C)e4xy_p = (Ax^2+Bx+C)e^{4x}. Za y=Pe4xy = Pe^{4x}: y″−2y′−3y=[P″+6P′+5P]e4xy''-2y'-3y = \big[P'' + 6P' + 5P\big]e^{4x}:

5Ax2+(12A+5B)x+(2A+6B+5C)=25x2⇒A=5,B=−12,C=6255Ax^2 + (12A + 5B)x + (2A + 6B + 5C) = 25x^2 \;\Longrightarrow\; A = 5,\; B = -12,\; C = \frac{62}{5}

y=C1e3x+C2e−x+(5x2−12x+625)e4xy = C_1e^{3x} + C_2e^{-x} + \Big(5x^2 - 12x + \dfrac{62}{5}\Big)e^{4x}

Zadatak 2a [3 poena]. Apsolutna/uslovna konvergencija ∑n=1∞(−1)nn2+1(n+1)4\displaystyle\sum_{n=1}^{\infty}(-1)^n\frac{n^2+1}{(n+1)^4}

Prikaži rešenje

Apsolutni red: n2+1(n+1)4∼1n2\frac{n^2+1}{(n+1)^4} \sim \frac{1}{n^2}; 2. poredbeni sa 1n2\frac{1}{n^2}: ℓ=1\ell = 1, a ∑1n2\sum\frac{1}{n^2} konvergira.

Apsolutno konvergira (pa Lajbnic nije ni potreban!)

Zadatak 2b [4 poena]. Uniformna konvergencija ∑n=1∞(sin⁡xcos⁡x)nn+3n\displaystyle\sum_{n=1}^{\infty}\frac{(\sin x\cos x)^n}{n + 3^n}, x∈ℝx\in\mathbb{R}

Prikaži rešenje

|sin⁡xcos⁡x|=|sin⁡2x|2≤12|\sin x\cos x| = \frac{|\sin 2x|}{2} \le \frac12 i n+3n≥3nn + 3^n \ge 3^n:

|fn(x)|≤(1/2)n3n=16n|f_n(x)| \le \frac{(1/2)^n}{3^n} = \frac{1}{6^n}

∑16n\sum\frac{1}{6^n} je konvergentan geometrijski red → po Vajerštrasu:

red uniformno konvergira na ℝ\mathbb{R}

Zadatak 2v [6 poena]. Interval konvergencije ∑n=1∞3nxn2n2+2\displaystyle\sum_{n=1}^{\infty}\frac{3^nx^n}{2n^2+2}

Prikaži rešenje

R=lim⁡|anan+1|=lim⁡3n(2(n+1)2+2)3n+1(2n2+2)=13R = \lim\Big|\frac{a_n}{a_{n+1}}\Big| = \lim\frac{3^n\big(2(n+1)^2+2\big)}{3^{n+1}(2n^2+2)} = \frac13

Konvergira za −13<x<13-\frac13 < x < \frac13. Krajevi: x=±13x = \pm\frac13 daju ∑(±1)n2n2+2\sum\frac{(\pm1)^n}{2n^2+2} — apsolutno konvergira (poredbeni sa 1n2\frac{1}{n^2}).

D=[−13,13]D = \Big[-\dfrac13, \dfrac13\Big]

Drugi deo

Zadatak 1 [6 poena]. Uslovni ekstremumi f=x2+xy+y2f = x^2+xy+y^2 uz x2+y2=1x^2+y^2 = 1  ·  identičan popravnom drugog 21/22 (K4, zadatak 1)!

Prikaži rešenje

Isto rešenje kao K4 zadatak 1: λ=−12\lambda = -\frac12 daje minimum f=12f = \frac12 u (±22,∓22)\big({\pm\frac{\sqrt2}{2}}, {\mp\frac{\sqrt2}{2}}\big); λ=−32\lambda = -\frac32 maksimum f=32f = \frac32 u (±22,±22)\big({\pm\frac{\sqrt2}{2}}, {\pm\frac{\sqrt2}{2}}\big).

fmin=12f_{\min} = \frac12, fmax=32f_{\max} = \frac32

Zadatak 2 [6 poena]. ∭Vxyzdxdydz\displaystyle\iiint_V xyz\,dxdydz; VV: x,y,z≥0x,y,z \ge 0, x2+y2+z2≤1x^2+y^2+z^2 \le 1 (osmina lopte)

Prikaži rešenje

Sferne koordinate; prvi oktant: φ∈[0,π2]\varphi\in[0,\frac{\pi}{2}], θ∈[0,π2]\theta\in[0,\frac{\pi}{2}], ρ∈[0,1]\rho\in[0,1]:

xyz⋅ρ2sin⁡θ=ρ5cos⁡φsin⁡φsin⁡3θcos⁡θxyz\cdot\rho^2\sin\theta = \rho^5\cos\varphi\sin\varphi\,\sin^3\theta\cos\theta

I=∫01ρ5dρ⏟1/6⋅∫0π/2sin⁡φcos⁡φdφ⏟1/2⋅∫0π/2sin⁡3θcos⁡θdθ⏟1/4I = \underbrace{\int_0^1\rho^5d\rho}_{1/6}\cdot\underbrace{\int_0^{\pi/2}\sin\varphi\cos\varphi\,d\varphi}_{1/2}\cdot\underbrace{\int_0^{\pi/2}\sin^3\theta\cos\theta\,d\theta}_{1/4}

I=148I = \dfrac{1}{48}

Zadatak 3 [5 poena]. ∫Cxyzds\displaystyle\int_C xyz\,ds; CC: x=tx = t, y=8t33y = \dfrac{\sqrt{8t^3}}{3}, z=t22z = \dfrac{t^2}{2}, od A(0,0,0)A(0,0,0) do B(1,223,12)B\big(1, \frac{2\sqrt2}{3}, \frac12\big)

Prikaži rešenje

y=223t3/2y = \frac{2\sqrt2}{3}t^{3/2} → y′=2t1/2y' = \sqrt2\,t^{1/2}, x′=1x' = 1, z′=tz' = t; ključno — potkorena veličina je potpun kvadrat:

ds=1+2t+t2dt=(1+t)dtds = \sqrt{1 + 2t + t^2}\,dt = (1+t)\,dt

Integrand: xyz=t⋅223t3/2⋅t22=23t9/2xyz = t\cdot\frac{2\sqrt2}{3}t^{3/2}\cdot\frac{t^2}{2} = \frac{\sqrt2}{3}t^{9/2}; granice t:0→1t: 0 \to 1 (u t=1t=1 je tačno BB ✓):

I=23∫01t9/2(1+t)dt=23(211+213)=23⋅48143I = \frac{\sqrt2}{3}\int_0^1t^{9/2}(1+t)\,dt = \frac{\sqrt2}{3}\Big(\frac{2}{11} + \frac{2}{13}\Big) = \frac{\sqrt2}{3}\cdot\frac{48}{143}

I=162143I = \dfrac{16\sqrt2}{143}

Zadatak 4 [6 poena]. ∬Sx2z2dS\displaystyle\iint_S x^2z^2\,dS; konus z=x2+y2z = \sqrt{x^2+y^2} između z=az = a i z=bz = b  ·  identičan K3, zadatak 4!

Prikaži rešenje

Isto kao K3 zadatak 4: dS=2dxdydS = \sqrt2\,dxdy, projekcija prsten a2≤x2+y2≤b2a^2 \le x^2+y^2 \le b^2, x2z2=ρ4cos⁡2φx^2z^2 = \rho^4\cos^2\varphi:

I=2π(b6−a6)6I = \dfrac{\sqrt2\,\pi(b^6 - a^6)}{6}

Prvi kolokvijum — 23. 11. 2018. (stariji format)

Stariji format: 3 zadatka, uključuje i Furijeov red. Zadatak 1a je najteži Lagranž koji se pojavio — dobra „gornja granica” težine.

Zadatak 1a. y=xy′+2x1+y′2\;y = xy' + 2x\sqrt{1 + y'^2}  ·  Lagranžova (zbog 2x2x NIJE Klerova!)

Prikaži rešenje

y=x(p+21+p2)⏟f(p)y = x\underbrace{\big(p + 2\sqrt{1+p^2}\big)}_{f(p)} — Lagranžova sa φ=0\varphi = 0. Diferenciraj po xx:

p=f(p)+xf′(p)dpdx⇒−21+p2=x(1+2p1+p2)dpdxp = f(p) + xf'(p)\frac{dp}{dx} \;\Longrightarrow\; -2\sqrt{1+p^2} = x\Big(1 + \frac{2p}{\sqrt{1+p^2}}\Big)\frac{dp}{dx}

Razdvoji (x(p)x(p)):

dxx=−[121+p2+p1+p2]dp⇒ln⁡|x|=−12ln⁡(p+1+p2)−12ln⁡(1+p2)+ln⁡c\frac{dx}{x} = -\Big[\frac{1}{2\sqrt{1+p^2}} + \frac{p}{1+p^2}\Big]dp \;\Longrightarrow\; \ln|x| = -\frac12\ln\big(p+\sqrt{1+p^2}\big) - \frac12\ln(1+p^2) + \ln c

(∫dp1+p2=ln⁡(p+1+p2)\int\frac{dp}{\sqrt{1+p^2}} = \ln(p+\sqrt{1+p^2}) — tablični!)

x=c(p+1+p2)(1+p2),y=x(p+21+p2)x = \dfrac{c}{\sqrt{\big(p+\sqrt{1+p^2}\,\big)(1+p^2)}}, \qquad y = x\big(p + 2\sqrt{1+p^2}\big) (parametarski)

Zadatak 1b. y″+y′−2y=(x2−1)e2x+cos⁡2x\;y'' + y' - 2y = (x^2-1)e^{2x} + \cos 2x

Prikaži rešenje

KJ: r2+r−2=(r−1)(r+2)r^2 + r - 2 = (r-1)(r+2): yh=C1ex+C2e−2xy_h = C_1e^x + C_2e^{-2x}.

1° (x2−1)e2x(x^2-1)e^{2x}: a=2a = 2 nije koren → yp1=(Ax2+Bx+C)e2xy_{p_1} = (Ax^2+Bx+C)e^{2x}; za y=Pe2xy = Pe^{2x}: L(y)=[P″+5P′+4P]e2xL(y) = [P'' + 5P' + 4P]e^{2x}:

4A=1,10A+4B=0,2A+5B+4C=−1⇒A=14,B=−58,C=13324A = 1,\quad 10A + 4B = 0,\quad 2A + 5B + 4C = -1 \;\Longrightarrow\; A = \frac14,\; B = -\frac58,\; C = \frac{13}{32}

2° cos⁡2x\cos 2x: 2i2i nije koren → yp2=Dcos⁡2x+Esin⁡2xy_{p_2} = D\cos2x + E\sin2x: sistem −6D+2E=1-6D + 2E = 1, −2D−6E=0-2D - 6E = 0 → D=−320D = -\frac{3}{20}, E=120E = \frac{1}{20}.

y=C1ex+C2e−2x+(x24−5x8+1332)e2x−320cos⁡2x+120sin⁡2xy = C_1e^x + C_2e^{-2x} + \Big(\frac{x^2}{4} - \frac{5x}{8} + \frac{13}{32}\Big)e^{2x} - \frac{3}{20}\cos2x + \frac{1}{20}\sin2x

(Na fotografiji roka rukom su dopisani upravo 1332\frac{13}{32}, −320-\frac{3}{20}, 120\frac{1}{20} — poklapanje ✓)

Zadatak 2a. Konvergencija ∑n=1∞3n⋅n!nn\displaystyle\sum_{n=1}^{\infty}\frac{3^n\cdot n!}{n^n}  ·  treći put isti red (i 2022!)

Prikaži rešenje

Dalamber → ℓ=3e>1\ell = \frac{3}{e} > 1 → divergira (ceo račun u K1, zadatak 2a)

Zadatak 2b. Apsolutna/uslovna konvergencija ∑n=1∞(−1)n+11−cos⁡1n\displaystyle\sum_{n=1}^{\infty}(-1)^{n+1}\sqrt{1 - \cos\frac1n}

Prikaži rešenje

Identitet poluugla: 1−cos⁡1n=2sin⁡212n1 - \cos\frac1n = 2\sin^2\frac{1}{2n}, pa an=2sin⁡12n∼22n=12na_n = \sqrt2\,\sin\frac{1}{2n} \sim \frac{\sqrt2}{2n} = \frac{1}{\sqrt2\,n}.

Apsolutni: 2. poredbeni sa 1n\frac1n (ℓ=12\ell = \frac{1}{\sqrt2}) → divergira. Lajbnic: sin⁡12n\sin\frac{1}{2n} opada i teži 0 ✓.

Uslovno konvergira

Zadatak 3. f(x)={x,0≤x≤12−x,1<x≤2f(x) = \begin{cases}x, & 0\le x\le 1\\ 2-x, & 1 < x\le 2\end{cases} razviti u Furijeov red po sinusima  ·  identičan zadatku F4 sa 5. vežbi!

Prikaži rešenje

Neparno produženje, ℓ=2\ell = 2: bn=∫01xsin⁡nπx2dx+∫12(2−x)sin⁡nπx2dx=8n2π2sin⁡nπ2b_n = \int_0^1x\sin\frac{n\pi x}{2}dx + \int_1^2(2-x)\sin\frac{n\pi x}{2}dx = \frac{8}{n^2\pi^2}\sin\frac{n\pi}{2}; preživljavaju neparni:

f(x)=8π2∑n=1∞(−1)n−1(2n−1)2sin⁡(2n−1)πx2f(x) = \dfrac{8}{\pi^2}\sum\limits_{n=1}^{\infty}\dfrac{(-1)^{n-1}}{(2n-1)^2}\sin\dfrac{(2n-1)\pi x}{2}

Popravni kolokvijum — 17. 6. 2020. (oba dela)

Prvi deo

Zadatak 1 [5 poena]. y″−4y′+3y=e3x+sin⁡3x\;y'' - 4y' + 3y = e^{3x} + \sin 3x

Prikaži rešenje

KJ: (r−1)(r−3)=0(r-1)(r-3) = 0: yh=C1ex+C2e3xy_h = C_1e^x + C_2e^{3x}.

1° e3xe^{3x}: a=3a = 3 jeste koren (p=1p=1) → yp1=Axe3xy_{p_1} = Axe^{3x}: uvrštavanjem 2Ae3x=e3x⇒A=122Ae^{3x} = e^{3x} \Rightarrow A = \frac12.

2° sin⁡3x\sin 3x: 3i3i nije koren → yp2=Bcos⁡3x+Dsin⁡3xy_{p_2} = B\cos3x + D\sin3x: sistem −6B−12D=0-6B - 12D = 0, 12B−6D=112B - 6D = 1 → B=115B = \frac{1}{15}, D=−130D = -\frac{1}{30}.

y=C1ex+C2e3x+x2e3x+115cos⁡3x−130sin⁡3xy = C_1e^x + C_2e^{3x} + \frac{x}{2}e^{3x} + \frac{1}{15}\cos3x - \frac{1}{30}\sin3x

Zadatak 2a [3 poena]. Konvergencija ∑n=1∞2n2n−1\displaystyle\sum_{n=1}^{\infty}\frac{2^n}{2n-1}  ·  zamka!

Prikaži rešenje

Potreban uslov: an=2n2n−1→+∞≠0a_n = \frac{2^n}{2n-1} \to +\infty \neq 0 (eksponencijalna pobeđuje linearnu).

Red divergira — bez ijednog kriterijuma, samo potreban uslov!

Zadatak 2b [3 poena]. Apsolutna/uslovna konvergencija ∑n=1∞(−1)nn2+1+n\displaystyle\sum_{n=1}^{\infty}\frac{(-1)^n}{\sqrt{n^2+1}+n}

Prikaži rešenje

an=1n2+1+n∼12na_n = \frac{1}{\sqrt{n^2+1}+n} \sim \frac{1}{2n}: apsolutni divergira (2. poredbeni sa 1n\frac1n, ℓ=12\ell = \frac12). Lajbnic: imenilac raste → an↓0a_n\downarrow0 ✓.

Uslovno konvergira

Zadatak 3 [6 poena]. Interval konvergencije ∑n=1∞(−1)n(x+3)n2n⋅n\displaystyle\sum_{n=1}^{\infty}\frac{(-1)^n(x+3)^n}{2^n\cdot n}

Prikaži rešenje

R=lim⁡2n+1(n+1)2nn=2R = \lim\frac{2^{n+1}(n+1)}{2^nn} = 2; centar x0=−3x_0 = -3: konvergira za −5<x<−1-5 < x < -1. Krajevi:

  • x=−1x = -1: ∑(−1)n2n2nn=∑(−1)nn\sum(-1)^n\frac{2^n}{2^nn} = \sum\frac{(-1)^n}{n} — Lajbnic → konvergira (uslovno).
  • x=−5x = -5: ∑(−1)n(−2)n2nn=∑1n\sum(-1)^n\frac{(-2)^n}{2^nn} = \sum\frac1n — harmonijski → divergira.

D=(−5,−1]D = (-5, -1] (pazi: (−1)n(−1)n=1(-1)^n(-1)^n = 1!)

Drugi deo

Zadatak 1 [6 poena]. Ekstremne vrednosti f(x,y)=2x3+xy2+5x2+y2f(x,y) = 2x^3 + xy^2 + 5x^2 + y^2  ·  LOKALNI (bez uslova!)

Prikaži rešenje

fx=6x2+y2+10x=0,fy=2xy+2y=2y(x+1)=0f_x = 6x^2 + y^2 + 10x = 0, \qquad f_y = 2xy + 2y = 2y(x+1) = 0

Iz druge: y=0y = 0 ili x=−1x = -1. y=0y = 0: 6x2+10x=0⇒x=06x^2+10x = 0 \Rightarrow x = 0 ili x=−53x = -\frac53. x=−1x = -1: 6+y2−10=0⇒y=±26 + y^2 - 10 = 0 \Rightarrow y = \pm2.

Četiri stacionarne tačke; fxx=12x+10f_{xx} = 12x+10, fxy=2yf_{xy} = 2y, fyy=2x+2f_{yy} = 2x+2:

  • (0,0)(0,0): A=10A = 10, B=0B = 0, C=2C = 2: AC−B2=20>0AC-B^2 = 20 > 0, A>0A>0 → min, f=0f = 0.
  • (−53,0)\big({-\frac53}, 0\big): A=−10A = -10, B=0B = 0, C=−43C = -\frac43: AC−B2=403>0AC-B^2 = \frac{40}{3} > 0, A<0A<0 → max, f=12527f = \frac{125}{27}.
  • (−1,±2)(-1, \pm2): A=−2A = -2, B=±4B = \pm4, C=0C = 0: AC−B2=−16<0AC-B^2 = -16 < 0 → sedla.

min f(0,0)=0f(0,0) = 0; max f(−53,0)=12527f\big({-\frac53},0\big) = \frac{125}{27}; sedla u (−1,±2)(-1,\pm2)

Zadatak 2 [5 poena]. ∬D(x2+y2)dxdy\displaystyle\iint_D(x^2+y^2)\,dxdy; DD: krug x2+y2=2xx^2+y^2 = 2x

Prikaži rešenje

Dopuna do kvadrata: (x−1)2+y2≤1(x-1)^2 + y^2 \le 1; u polarnim ρ≤2cos⁡φ\rho \le 2\cos\varphi, φ∈[−π2,π2]\varphi\in\big[{-\frac{\pi}{2}}, \frac{\pi}{2}\big]:

∬=∫−π/2π/2∫02cos⁡φρ2⋅ρdρdφ=∫−π/2π/2(2cos⁡φ)44dφ=8∫0π/2cos⁡4φdφ=8⋅3π16\iint = \int_{-\pi/2}^{\pi/2}\int_0^{2\cos\varphi}\rho^2\cdot\rho\,d\rho\,d\varphi = \int_{-\pi/2}^{\pi/2}\frac{(2\cos\varphi)^4}{4}d\varphi = 8\int_0^{\pi/2}\cos^4\varphi\,d\varphi = 8\cdot\frac{3\pi}{16}

3π2\dfrac{3\pi}{2} (Valis: ∫0π/2cos⁡4=3π16\int_0^{\pi/2}\cos^4 = \frac{3\pi}{16})

Zadatak 3 [6 poena]. ∬S(xy+yz+xz)dS\displaystyle\iint_S(xy + yz + xz)\,dS; SS: deo konusa z=x2+y2z = \sqrt{x^2+y^2} unutar cilindra x2+y2=4xx^2+y^2 = 4x

Prikaži rešenje

dS=2dxdydS = \sqrt2\,dxdy; projekcija: (x−2)2+y2≤4(x-2)^2+y^2 \le 4, simetrična oko xx-ose. Uz z=x2+y2z = \sqrt{x^2+y^2}:

xy+yz+xz=xy⏟neparno po y→0+yx2+y2⏟neparno po y→0+xx2+y2xy + yz + xz = \underbrace{xy}_{\text{neparno po }y\,\to\,0} + \underbrace{y\sqrt{x^2+y^2}}_{\text{neparno po }y\,\to\,0} + x\sqrt{x^2+y^2}

Polarne (ρ≤4cos⁡φ\rho \le 4\cos\varphi, φ∈[−π2,π2]\varphi\in[-\frac{\pi}{2},\frac{\pi}{2}]): xx2+y2⋅ρ=ρ3cos⁡φx\sqrt{x^2+y^2}\cdot\rho = \rho^3\cos\varphi:

I=2∫−π/2π/2cos⁡φ⋅(4cos⁡φ)44dφ=642∫−π/2π/2cos⁡5φdφ=642⋅1615I = \sqrt2\int_{-\pi/2}^{\pi/2}\cos\varphi\cdot\frac{(4\cos\varphi)^4}{4}\,d\varphi = 64\sqrt2\int_{-\pi/2}^{\pi/2}\cos^5\varphi\,d\varphi = 64\sqrt2\cdot\frac{16}{15}

I=1024215I = \dfrac{1024\sqrt2}{15} (Valis: ∫0π/2cos⁡5=815\int_0^{\pi/2}\cos^5 = \frac{8}{15})

🆕 Probni kolokvijum A — prvi (sveži zadaci)

Generisan tačno po obrascu rokova 2018–2025, ali sa zadacima kojih nema ni na jednom roku ni u skripti — za pošteno testiranje transfera. Radi pod satom (90 min), bez materijala.

Zadatak 1a [5 poena]. Odrediti opšte rešenje: y=2xy′+y′2\;y = 2xy' + y'^2

Prikaži rešenje

Lagranžova (f(p)=2p≠pf(p) = 2p \neq p, φ(p)=p2\varphi(p) = p^2). Smena y′=py' = p, diferenciraj po xx:

p=2p+(2x+2p)dpdx⇒−p=2(x+p)dpdx⇒x′+2px=−2(linearna po x(p))p = 2p + (2x + 2p)\frac{dp}{dx} \;\Longrightarrow\; -p = 2(x+p)\frac{dp}{dx} \;\Longrightarrow\; x' + \frac{2}{p}x = -2 \quad(\text{linearna po } x(p))

x=uvx = uv: iz v′+2vp=0v' + \frac{2v}{p} = 0: v=p−2v = p^{-2}; iz u′p−2=−2u'p^{-2} = -2: u=−2p33+cu = -\frac{2p^3}{3} + c:

x=cp2−2p3,y=2xp+p2=2cp−p23x = \dfrac{c}{p^2} - \dfrac{2p}{3}, \qquad y = 2xp + p^2 = \dfrac{2c}{p} - \dfrac{p^2}{3} (parametarski)

Provera: dy/dpdx/dp=−2c/p2−2p/3−2c/p3−2/3=p=y′\frac{dy/dp}{dx/dp} = \frac{-2c/p^2 - 2p/3}{-2c/p^3 - 2/3} = p = y' ✓

Zadatak 1b [5 poena]. y″+4y=8x+sin⁡2x\;y'' + 4y = 8x + \sin 2x

Prikaži rešenje

KJ: r2+4=0⇒r=±2ir^2 + 4 = 0 \Rightarrow r = \pm 2i: yh=C1cos⁡2x+C2sin⁡2xy_h = C_1\cos 2x + C_2\sin 2x. Superpozicija:

1° Q1=8xQ_1 = 8x (a=0a = 0 nije koren): yp1=Ax+By_{p_1} = Ax + B: 4Ax+4B=8x⇒A=2\;4Ax + 4B = 8x \Rightarrow A = 2, B=0B = 0.

2° Q2=sin⁡2xQ_2 = \sin 2x: α+iβ=2i\alpha + i\beta = 2i JESTE koren (p=1p=1) → rezonanca: yp2=x(Ccos⁡2x+Dsin⁡2x)y_{p_2} = x(C\cos 2x + D\sin 2x). Računom: C=−14C = -\frac14, D=0D = 0.

y=C1cos⁡2x+C2sin⁡2x+2x−x4cos⁡2xy = C_1\cos 2x + C_2\sin 2x + 2x - \dfrac{x}{4}\cos 2x

Provera yp2y_{p_2}: za y=−x4cos⁡2xy = -\frac x4\cos2x: y″=sin⁡2x+xcos⁡2xy'' = \sin2x + x\cos2x, pa y″+4y=sin⁡2xy'' + 4y = \sin2x ✓

Zadatak 2a [3 poena]. Ispitati konvergenciju ∑n=1∞2nn!nn\displaystyle\sum_{n=1}^{\infty}\frac{2^n\,n!}{n^n}

Prikaži rešenje

Dalamber (isti račun kao za čuveni 3nn!nn\frac{3^nn!}{n^n}, ali sa dvojkom!):

an+1an=2(1+1n)n→2e≈0,74<1\frac{a_{n+1}}{a_n} = \frac{2}{\big(1+\frac1n\big)^n} \longrightarrow \frac2e \approx 0{,}74 < 1

Red konvergira — pazi: sa trojkom divergira (3e>1\frac3e>1), sa dvojkom konvergira. Isti oblik, suprotan zaključak — zato se ne uči odgovor napamet nego račun!

Zadatak 2b [4 poena]. Ispitati apsolutnu i uslovnu konvergenciju ∑n=1∞(−1)nnn2+2\displaystyle\sum_{n=1}^{\infty}(-1)^n\frac{n}{n^2+2}

Prikaži rešenje

Apsolutni: nn2+2∼1n\frac{n}{n^2+2} \sim \frac1n; 2. poredbeni sa 1n\frac1n: ℓ=1\ell = 1, harmonijski divergira ⇒ nije apsolutna.

Lajbnic: f(x)=xx2+2f(x) = \frac{x}{x^2+2}, f′(x)=2−x2(x2+2)2<0f'(x) = \frac{2 - x^2}{(x^2+2)^2} < 0 za x>2x > \sqrt2 → opada od n=2n = 2 (konačno mnogo članova ne smeta); an→0a_n \to 0 ✓.

Uslovno konvergira

Zadatak 2v [6 poena]. Odrediti interval konvergencije ∑n=1∞(x+1)nn⋅3n\displaystyle\sum_{n=1}^{\infty}\frac{(x+1)^n}{n\cdot 3^n}

Prikaži rešenje

R=lim⁡|anan+1|=lim⁡(n+1)3n+1n⋅3n=3R = \lim\Big|\frac{a_n}{a_{n+1}}\Big| = \lim\frac{(n+1)3^{n+1}}{n\cdot3^n} = 3

Centar x0=−1x_0 = -1: konvergira za −4<x<2-4 < x < 2. Krajevi:

  • x=2x = 2: ∑3nn3n=∑1n\sum\frac{3^n}{n3^n} = \sum\frac1n — divergira.
  • x=−4x = -4: ∑(−3)nn3n=∑(−1)nn\sum\frac{(-3)^n}{n3^n} = \sum\frac{(-1)^n}{n} — Lajbnic → konvergira.

D=[−4,2)D = [-4, 2)

🆕 Probni kolokvijum B — drugi (sveži zadaci)

Zadatak 1 [6 poena]. Odrediti uslovne ekstremume f(x,y)=3x+4yf(x,y) = 3x + 4y uz x2+y2=25x^2 + y^2 = 25

Prikaži rešenje

F=3x+4y+λ(x2+y2−25)F = 3x + 4y + \lambda(x^2+y^2-25): 3+2λx=0\;3 + 2\lambda x = 0, 4+2λy=04 + 2\lambda y = 0 → x=−32λx = -\frac{3}{2\lambda}, y=−2λy = -\frac{2}{\lambda}.

Uslov: 94λ2+4λ2=25⇒254λ2=25⇒λ=±12\frac{9}{4\lambda^2} + \frac{4}{\lambda^2} = 25 \Rightarrow \frac{25}{4\lambda^2} = 25 \Rightarrow \lambda = \pm\frac12.

  • λ=12\lambda = \frac12: M1(−3,−4)M_1(-3, -4), d2F>0d^2F > 0 → min, f=−25f = -25.
  • λ=−12\lambda = -\frac12: M2(3,4)M_2(3, 4), d2F<0d^2F < 0 → max, f=25f = 25.

fmin=−25f_{\min} = -25, fmax=25f_{\max} = 25 (kontrola: ±∥(3,4)∥⋅5=±25\pm\|(3,4)\|\cdot 5 = \pm 25 ✓)

Zadatak 2 [6 poena]. Izračunati zapreminu tela ograničenog paraboloidom z=x2+y2z = x^2+y^2 i ravni z=4z = 4, pri čemu je x≥0x \ge 0

Prikaži rešenje

Presek: x2+y2=4x^2+y^2 = 4; zbog x≥0x \ge 0 projekcija je polukrug (φ∈[−π2,π2]\varphi\in[-\frac{\pi}{2}, \frac{\pi}{2}] — pazi, ovog puta desni!):

V=∫−π/2π/2dφ∫02(4−ρ2)ρdρ=π(2ρ2−ρ44)|02=π(8−4)V = \int_{-\pi/2}^{\pi/2}d\varphi\int_0^2(4-\rho^2)\rho\,d\rho = \pi\Big(2\rho^2 - \frac{\rho^4}{4}\Big)\Big|_0^2 = \pi(8-4)

V=4πV = 4\pi (ceo krug bi dao 8π8\pi — uslov x≥0x\ge0 prepolovljava!)

Zadatak 3 [5 poena]. Izračunati ∫Czds\displaystyle\int_C z\,ds, gde je CC: x=cos⁡tx = \cos t, y=sin⁡ty = \sin t, z=2tz = 2t, t∈[0,π]t\in[0, \pi]

Prikaži rešenje

ds=sin⁡2t+cos⁡2t+4dt=5dtds = \sqrt{\sin^2t + \cos^2t + 4}\,dt = \sqrt5\,dt

I=∫0π2t⋅5dt=5t2|0πI = \int_0^{\pi}2t\cdot\sqrt5\,dt = \sqrt5\,t^2\Big|_0^{\pi}

I=5π2I = \sqrt5\,\pi^2

Zadatak 4 [6 poena]. Izračunati ∬SzdS\displaystyle\iint_S z\,dS, gde je SS deo konusa z=x2+y2z = \sqrt{x^2+y^2} između ravni z=1z = 1 i z=2z = 2

Prikaži rešenje

Za konus: dS=2dxdydS = \sqrt2\,dxdy; projekcija: prsten 1≤x2+y2≤41 \le x^2+y^2 \le 4; na konusu z=ρz = \rho:

I=2∫02πdφ∫12ρ⋅ρdρ=2⋅2π⋅ρ33|12=22π⋅73I = \sqrt2\int_0^{2\pi}d\varphi\int_1^2\rho\cdot\rho\,d\rho = \sqrt2\cdot2\pi\cdot\frac{\rho^3}{3}\Big|_1^2 = 2\sqrt2\pi\cdot\frac{7}{3}

I=142π3I = \dfrac{14\sqrt2\,\pi}{3}

Posle simulacije

Za svaki zadatak gde nisi uzeo pune poene, u skripti imaš isti tip: Lagranžova/Klerova/Rikatijeva → S1 §2; LDJVR + rezonanca → S1 §3; kriterijumi i interval konvergencije → S1 §4–5; Furije → S1 §5; uslovni/lokalni ekstremumi → S2 §7; dvojni/trojni → S2 §8; krivolinijski i površinski 1. vrste → S2 §9. Uradi po 2–3 zadatka tog tipa i vrati se na sledeću simulaciju.

Raspodela za plan: Dan 10 → K1 (2022), pa Probni A ako K1 prođe glatko; Dan 19 → K3 (2022) + Probni B; Dan 20 → K2 + K4 (popravni 2022). Ostali rokovi (K5–K9) za dodatne simulacije — najvredniji je K7 (rok 22.10.2025, najnoviji format).