An inductor of inductance L=400mH and resistors of resistances R1=2Ω and R2=2Ω are connected to a battery of emf 12V as shown in the figure. The internal resistance of the battery is negligible. The switch S is closed at t=0. The potential drop across L as a function of time is :
6e⁻ᵗ/⁰·²V
12te⁻ᵗ/⁰·²V
12e⁻ᵗ/⁰·²V
6 (1−e⁻ᵗ/⁰·²)V
Solution:
I=ε/R=12/2=6A ε=L(dI/dt)+R2I2 I2=I0(1−e⁻ᵗ/tc) ⇒I0=ε/R2=12/2=6A tc=L/R=400×10⁻³=0.2 I2=6(1−e⁻ᵗ/⁰·²) Potential drop across L=ε−R2I2=12−2×6(1−e⁻ᵗ/⁰·²)=12e⁻ᵗ/⁰·²V