Due to Kirchhoff's law:
U L + U R + U C = E U_L+U_R+U_C=E U L â + U R â + U C â = E (1)
where
U L = L d i d t U_L=L\frac{di}{dt} U L â = L d t d i â ; U R = i R U_R=iR U R â = i R ; U C = 1 C ⍠i d t U_C=\frac1C\int idt U C â = C 1 â ⍠i d t .
Let's differentiate (1):
L d 2 i d t 2 + R d i d t + 1 C i = 0 L\frac{d^2i}{dt^2}+R\frac{di}{dt}+\frac 1C i=0 L d t 2 d 2 i â + R d t d i â + C 1 â i = 0
d 2 i d t 2 + R L d i d t + 1 L C i = 0 \frac{d^2i}{dt^2}+\frac RL\frac{di}{dt}+\frac {1}{LC} i=0 d t 2 d 2 i â + L R â d t d i â + L C 1 â i = 0
Characteristic equation:
Îť 2 + R L Îť + 1 L C = 0 \lambda^2+\frac RL\lambda+\frac {1}{LC}=0 Îť 2 + L R â Îť + L C 1 â = 0
R L = 20 0.05 = 400 \frac RL=\frac {20}{0.05}=400 L R â = 0.05 20 â = 400 ; 1 L C = 1 0.05 â
100 â
1 0 â 6 = 2 â
1 0 5 \frac {1}{LC}=\frac {1}{0.05\cdot 100\cdot 10^{-6}}=2\cdot10^5 L C 1 â = 0.05 â
100 â
1 0 â 6 1 â = 2 â
1 0 5 .
Îť 2 + 400 Îť + 2 â
1 0 5 = 0 \lambda^2+400\lambda+2\cdot 10^5=0 Îť 2 + 400 Îť + 2 â
1 0 5 = 0
Îť = â 200 Âą 400 j \lambda=-200\pm400j Îť = â 200 Âą 400 j , where j = â 1 j=\sqrt{-1} j = â 1 â .
i ( t ) = e â 200 t ( C 1 cos ⥠400 t + C 2 sin ⥠400 t ) i(t)=e^{-200t}(C_1 \cos {400t}+C_2 \sin {400t}) i ( t ) = e â 200 t ( C 1 â cos 400 t + C 2 â sin 400 t ) .
i ⣠t = 0 = C 1 = 0 ; i|_{t=0}=C_1=0; i ⣠t = 0 â = C 1 â = 0 ;
L d i d t ⣠t = 0 + R i ⣠t = 0 + U C ⣠t = 0 = E L\frac{di}{dt}|_{t=0}+Ri|_{t=0}+U_C|_{t=0}=E L d t d i â ⣠t = 0 â + R i ⣠t = 0 â + U C â ⣠t = 0 â = E (2)
U C ⣠t = 0 = 1 C Q ⣠t = 0 = 0 U_C|_{t=0}=\frac 1C Q|_{t=0}=0 U C â ⣠t = 0 â = C 1 â Q ⣠t = 0 â = 0 ; (3)
R i ⣠t = 0 = 0 Ri|_{t=0}=0 R i ⣠t = 0 â = 0 ; (4)
d i d t = C 2 e â 200 t ( â 200 â
sin ⥠400 t + 400 â
cos ⥠400 t ) \frac{di}{dt}=C_2e^{-200t}(-200\cdot\sin{400t}+400\cdot\cos{400t}) d t d i â = C 2 â e â 200 t ( â 200 â
sin 400 t + 400 â
cos 400 t ) ;
d i d t ⣠t = 0 = 400 â
C 2 \frac{di}{dt}|_{t=0}=400\cdot C_2 d t d i â ⣠t = 0 â = 400 â
C 2 â . (5)
Substitute (3), (4) and (5) into (2):
L â
400 â
C 2 = E L\cdot400\cdot C_2=E L â
400 â
C 2 â = E ;
C 2 = E 400 â
L = 100 400 â
0.05 = 5 C_2=\frac{E}{400\cdot L}=\frac{100}{400\cdot 0.05}=5 C 2 â = 400 â
L E â = 400 â
0.05 100 â = 5
i ( t ) = 5 â
e â 200 t â
sin ⥠400 t . i(t)=5\cdot e^{-200t}\cdot \sin{400t}. i ( t ) = 5 â
e â 200 t â
sin 400 t .
Q ( t ) = ⍠5 â
e â 200 t â
sin ⥠400 t d t = Q(t)=\int5\cdot e^{-200t}\cdot \sin{400t} dt= Q ( t ) = ⍠5 â
e â 200 t â
sin 400 t d t =
â 1 200 e â 200 t ( sin ⥠400 t + 2 cos ⥠400 t ) + C 3 -\frac{1}{200}e^{-200t}(\sin{400t}+2\cos{400t})+C_3 â 200 1 â e â 200 t ( sin 400 t + 2 cos 400 t ) + C 3 â ;
Q ⣠t = 0 = â 1 200 â
2 + C 3 = 0 Q|_{t=0}=-\frac{1}{200}\cdot2+C_3=0 Q ⣠t = 0 â = â 200 1 â â
2 + C 3 â = 0 ;
C 3 = 1 100 C_3=\frac{1}{100} C 3 â = 100 1 â
Q ( t ) = 1 200 [ 2 â e â 200 t ( sin ⥠400 t + 2 cos ⥠400 t ) ] Q(t)=\frac{1}{200}[2-e^{-200t}(\sin{400t}+2\cos{400t})] Q ( t ) = 200 1 â [ 2 â e â 200 t ( sin 400 t + 2 cos 400 t )] .
Answer:
i ( t ) = 5 â
e â 200 t â
sin ⥠400 t i(t)=5\cdot e^{-200t}\cdot \sin{400t} i ( t ) = 5 â
e â 200 t â
sin 400 t ;
Q ( t ) = 1 200 [ 2 â e â 200 t ( sin ⥠400 t + 2 cos ⥠400 t ) ] Q(t)=\frac{1}{200}[2-e^{-200t}(\sin{400t}+2\cos{400t})] Q ( t ) = 200 1 â [ 2 â e â 200 t ( sin 400 t + 2 cos 400 t )] .
Comments