Rešenja i načini rada zadataka sa kolokvijuma iz matematike 2017/2018
Ovde će biti prikazano na koji način smo došli do tačnih rešenja datih zadataka.
Zadatak br.1
Izracunati masu krive l: $$ x^2+y^2+z=4, x^2+y^2+z^2=4z $$ ako je gustina $$ ρ(x,y,z)= 10z+x^2+y^3 $$
Za ovaj zadatak prvo se određuje oblast u prostoru u kojoj se nalazi kriva – ona je definisana presekom površina
𝑥
^
2
+
𝑦
^
2
+
𝑧
=
4,
x
^
2
+
y
^
2
+
z
^
2
=
4 z
.
Zatim se vrši parametrizacija presečne krive, pomoću polarnih koordinata.
Nakon toga se izračunava element dužine
ds na osnovu parametarske jednačine krive.
Masa se određuje integralom duž krive:
∫
𝐿
𝜌
(
𝑥
,
𝑦
,
𝑧
)
.
Na kraju se u integral unosi konkretna gustina
ρ(x,y,z)=10z+x^
2
+y^
3
, pa se obavlja računanje integrala.
$$
\begin{aligned}
&\text { 1. } f: x^2+y^2+z=4, x^2+y^2+z^2=4 z \quad \rho(x, y, z)=10 z+x^2+y^3\\
&\begin{aligned}
& \left.\begin{array}{l}
z-4=-x^2-y^2 \\
4 z-z^2=x^2+y^2
\end{array}\right\}+ \\
& \begin{array}{l}
z-4=-x^2-y^2 \\
z-4+4 z-z^2-x^2-y^2+x^2+y^2
\end{array} \\
& -z^2+4 z+z-4=0 \\
& -z^2+5 z-4=0 \\
& z_{1 / 2}=\frac{-5 \pm \sqrt{25-16}}{-2} \\
& z_{1 / 2}=\frac{-5 \pm 3}{-2} \\
& z_1=1 \\
& z_2=4
\end{aligned}
\end{aligned}
$$
Prvi slučaj
$$
\begin{gathered}
\text { l: } x^2+y^2+1=4 \\
x^2+y^2=3 \\
x=\cos t \cdot \sqrt{3} \\
y=\sqrt{3} \sin t \\
z=+1 \\
d s=\sqrt{\left(\left(x^{\prime}(t)\right)^2+\left(y^{\prime}(t)\right)^2+\left(z^{\prime}(t)\right)^2 d t\right.} \\
x^{\prime}(t)=-1 \cdot \sin t \cdot \sqrt{3} \quad y^{\prime}(t)=\cos t \cdot \sqrt{3} \\
d s=\sqrt{3 \sin ^2 x+3 \cos ^2 x+0} \cdot d t=\sqrt{3} d t
\end{gathered}
$$
Drugi slučaj:
$$
\begin{aligned}
& l: x^2+y^2+4=4 \\
& x^2+y^2=0 \\
& x=\sqrt{0} \cdot \cos t=0 \\
& y=\sqrt{0} \cdot \sin t=0 \\
& z=4
\end{aligned}
$$
$$
d S=\sqrt{0+0+0} \cdot {d t}{=} 0 d t{=}0
$$
$$
\begin{aligned}
&\text { Prvi slucaj: }\\
&\begin{aligned}
& m=\int 1\left(10z+x^2+y^3\right) d s=\int_0^{2 \pi}\left(1+10+3 \sin ^2 t+3 \sqrt{3} \cos ^3 t\right) \sqrt{3} d t= \\
& =10 \sqrt{3} \int d t+3 \sqrt{3} \int \sin ^2 t d t+9-\int \cos^3 t d t= \\
& {\left[\int \sin ^2 t=\int \frac{1-\cos 2 t}{2} d t=\frac{1}{2} \int(1-\cos 2 t) d t=\frac{1}{2} \int d t-\frac{1}{2} \int \cos 2 t d t=\right.} \\
& \left.-\frac{1}{2}(t-\sin 2 t)\right]
\end{aligned}\\
&\begin{aligned}
& {\left[\int \cos ^3 t d t=\int \cos t \cdot \cos ^2 t d t=\int \cos t \cdot\left(1-\sin ^2 t\right) d t=\right.} \\
& =\left\{\begin{array}{l}
\sin t=z \\
\cos t d t=d z
\end{array}\right\}=\int\left(1-z^2\right) d z=\int d z-\int z^2 d z=z-\frac{z^3}{3}= \\
& \left.=\sin t-\frac{\sin ^3 t}{3}\right] \\
& =10 \sqrt{3} t+3 \sqrt{3} \cdot \frac{1}{2}(t-\sin 2 t)+\left.9\left(\sin t-\frac{\sin ^3 t}{3}\right)\right|_0 ^{2 \pi}= \\
& =10 \sqrt{3}+\sqrt{3}\left(\frac{1}{2} t-10 \sqrt{3} \cdot 2 \pi+3 \sqrt{3} \cdot \frac{1}{2}(2 \pi-0)+0\right. \\
& =(20 \sqrt{3}+3 \sqrt{3}) \pi=23 \sqrt{3} \cdot \pi
\end{aligned}
\end{aligned}
$$
$$
\begin{aligned}
&\text { Drugi slučaj: }\\
&\begin{aligned}
& m=\int l\left(10 z+x^2+y^3\right) d s \\
& d s=0 \Rightarrow m=0
\end{aligned}
\end{aligned}
$$
Zadatak br.2
Izracunati $$
\iint_D \ln \left(\sqrt{x^2+y^2}\right) dx\, dy
$$
gde je D oblast odredjena relacijama $$ \ 1 \leq x^2+y^2 \leq 4, y \cdot \sqrt{3} \geq x, y \geq 0 $$
Prelazi se na polarne koordinate i postavljaju se granice za ρ i φ, integral se izarazava u polarnim koordinatama i Jakobijan daje dodatni faktor ρ, pa se integral pretvara u ρlnρ. Integral se zatim racuna primenom parcijalne integracije.
$$
\iint_D \ln \left(\sqrt{x^2+y^2}\right) dx\, dy
$$
$$
\begin{aligned}
D= & \left\{f(x, y) \mid 1 \leq x^2+y^2 \leq 4, y \cdot \sqrt{3} \geq x, y \geq 0\right. \\
& x^2+y^2 \leq 4 \\
& x^2+y^2=4 \quad r_{A}=2\left(x_A, y_A\right)=(0,0) \\
& x^2+y^2 \geq 1 \\
& x^2+y^2=1 \quad r_B=1 \quad\left(x_B, y_B\right)=(0,0) \\
& y \cdot \sqrt{3} \geq x \Rightarrow y=\frac{x}{\sqrt{3}} \\
& y \geq 0 \Rightarrow y=0
\end{aligned}
$$
$$
\begin{array}{ll}
x=0, \text { onda je } & y=0 \\
x=1 & y=\frac{\sqrt{3}}{3} \\
x=2 & y=\frac{2 \sqrt{3}}{3}
\end{array}
$$
$$
\begin{gathered}
x=\rho \cos \varphi \\
y=\rho \sin \varphi \\
1 \le (\rho \cos \varphi)^2+(\rho \sin \varphi)^2 \le 4 \\
1 \le \rho^2 \cos^2 \varphi + \rho^2 \sin^2 \varphi \le 4 \\
1 \le \rho^2 \le 4 \\
1 \le \rho \le 2 \\
\Delta = \left\{ (\rho, \varphi) \mid 1 \le \rho \le 2, 0 \le \varphi \le \frac{\pi}{2} \right\}
\end{gathered}
$$
$$
\begin{aligned}
J &= \left|\begin{array}{ll}
x'_\rho & x'_\varphi \\
y'_\rho & y'_\varphi
\end{array}\right|
= \left|\begin{array}{cc}
\cos \varphi & -\rho \sin \varphi \\
\sin \varphi & \rho \cos \varphi
\end{array}\right|
= \rho \cos^2 \varphi + \rho \sin^2 \varphi = \rho \\
\iint_D \ln \left(\sqrt{x^2+y^2}\right) dx dy
&= \iint_\Delta \ln \left(\sqrt{\rho^2 \cos^2 \varphi + \rho^2 \sin^2 \varphi}\right) |\rho| d\varphi d\rho \\
&= \iint_\Delta \ln (\sqrt{\rho^2 (\cos^2 \varphi + \sin^2 \varphi)}) \rho d\varphi d\rho \\
&= \iint_\Delta \ln \rho \cdot \rho \, d\varphi d\rho \\
&= \int_0^{\pi/2} d\varphi \int_1^2 \rho \ln \rho \, d\rho
\end{aligned}
$$
$$
\begin{aligned}
\int_1^2 \rho \ln \rho \, d\rho
&= \left\{ \begin{array}{l}
u = \ln \rho \quad \Rightarrow du = \frac{1}{\rho} d\rho \\
dv = \rho d\rho \quad \Rightarrow v = \frac{\rho^2}{2}
\end{array} \right\} \\
&= \ln \rho \cdot \frac{\rho^2}{2} - \int \frac{\rho^2}{2} \cdot \frac{1}{\rho} d\rho \\
&= \frac{\rho^2}{2} \ln \rho - \frac{1}{4} \rho^2 \\
&= \left[ \frac{\rho^2}{2} \ln \rho - \frac{\rho^2}{4} \right]_1^2 \\
&= \frac{4}{2} \ln 2 - 1 - (0 - 1/4) \\
&= 3/2 \ln 2 + 3/4 \\
&= \frac{3}{2} (\ln 2 + 1/2)
\end{aligned}
$$
$$
\int_0^{\pi/2} d\varphi \cdot \frac{3}{2} (\ln 2 + 1/2) = \frac{3\pi}{4} (\ln 2 + 1/2)
$$