1.8.30 · HinglishElectromagnetism

LC circuit — oscillations (electrical analog of SHM)

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1.8.30 · Physics › Electromagnetism


Scratch se setup karna


Solution aur energy

Figure — LC circuit — oscillations (electrical analog of SHM)

Recall Feynman: ek 12-saal ke bacche ko explain karo

Ek swing imagine karo. Charge se bhara capacitor ek swing ki tarah hai jo poori tarah upar khichi hui ho — bahut "stored push," move nahi kar rahi. Chodo: yeh neechhe rush karta hai (current badhta hai) aur energy motion mein badal jaati hai. Sabse neechhe yeh sabse fast move kar raha hota hai (max current) lekin "height" (charge) zero hai. Yeh overshoot karta hai aur doosri taraf chadhta hai, capacitor ko ulta refill karta hai. Koi friction nahi toh hamesha ke liye swing karta rehta hai. Inductor swing ki "heaviness" hai jo ise neechhe se aage le jaata hai; capacitor woh "height" hai jo ise wapas kheenchti hai.


Flashcards

Ideal LC circuit ki differential equation kya hoti hai?
, yaani .
LC oscillations ki angular frequency kya hoti hai?
.
LC circuit ki period kya hoti hai?
.
Mechanical analogy mein mass ka role kaun play karta hai?
Inductance .
Mechanical analogy mein spring constant ka role kya play karta hai?
.
LC circuit mein position ka analog kya hai?
Capacitor par charge .
Velocity ka analog kya hai?
Current .
Charge aur current mein kitne phase ka fark hota hai?
(current max hota hai jab charge zero hota hai).
Ideal LC circuit hamesha kyun oscillate karta hai?
Ismein koi resistance nahi hoti, isliye total energy conserved rehti hai (koi dissipation nahi).
Capacitor aur inductor mein stored energy likhiye.
aur .
Period ke kitne fraction par energy equally share hoti hai?
par (aur odd multiples par), jahan .
Peak current ka peak charge se kya relation hai?
.

Connections

Concept Map

charged cap starts

stores electric energy

stores magnetic energy

V_C = q/C

V_L = L di/dt

sub i = dq/dt

matches SHM

term-by-term match

gives

solution

differentiate

energy swaps

LC circuit no R

Charge oscillates

Capacitor C

U_E = q^2 / 2C

Inductor L

U_B = L i^2 / 2

Kirchhoff loop V_C + V_L = 0

d2q/dt2 = -q / LC

SHM: x'' = -omega^2 x

q to x, L to m, 1/C to k

omega = 1 / sqrt(LC)

q = q0 cos(omega t)

i = -i0 sin(omega t) 90 deg phase