Key relationship
RC: Vc=V(1−e⁻ᵗ/ᴿᶜ); LR: I=V/R(1−e⁻ᴿᵗ/ᴸ); LC: Vc=Vcos(t/√LC).
Physics · Class 12
Switch among capacitor charging, inductor current rise and ideal energy exchange in an LC circuit. RC and LR approach a steady state; ideal LC continues oscillating.
Open the interactive experiment →RC-இல் தேக்கி மின்னழுத்தம் உயர்கிறது. LR-இல் மின்னோட்டம் உயர்கிறது. LC-இல் ஆற்றல் மின்புலத்துக்கும் காந்தப்புலத்துக்கும் மாறுகிறது.
RC: Vc=V(1−e⁻ᵗ/ᴿᶜ); LR: I=V/R(1−e⁻ᴿᵗ/ᴸ); LC: Vc=Vcos(t/√LC).
Switch among capacitor charging, inductor current rise and ideal energy exchange in an LC circuit. RC and LR approach a steady state; ideal LC continues oscillating.
RC and LR approach a DC steady state; ideal LC keeps exchanging energy. Resistance would damp that ideal LC oscillation.
Ideal initial conditions: RC uncharged, LR zero current, LC initially charged with zero current. LR voltage readout is across the inductor; LC has no resistance.
Use the controls and plotted relation to explain rc, lr and lc transients.
Try both scenarios, change one control, and predict the result before checking the graph and readouts.
Change one input while keeping the others fixed, as you would in a controlled experiment.
With R=100 Ω and C=100 µF, τ=0.01 s; after τ, a 12 V source gives Vc≈7.585 V.
The model connects rc, lr and lc transients with an observable reading. Check the equation and assumptions before applying it.
SI units · algebra · graph reading
After one RC time constant, a charging capacitor voltage is approximately?
63.2% of the supply voltage.
Course connection: Class XII Chapter 6. Consult the roadmap for CBSE, NEET, JEE Main and Advanced scope.