Answer:
D) e–Rt/LE) (1 – e–Rt/L)
Step-by-step explanation:
After some time t the current does not passing through the circuit
=>so the back emf is zero
=>here the inductor opposes decay of the circuit
-Ldi/dt=Ri
di/dt=-R/Li
di/i=-R/Ldt
now we applying the integration on both sides
log i=-R/Lt+C
here t=0=>i=io
Log io=C
=>Log i=-R/L×t+Log io
logi-Log io=-R/L×t
Log[i/io]=-R/L*t
i/io=e^-Rt/L
i=ioe^-Rt/L
the option D is correc