A LCR circuit behaves like a damped harmonic oscillator. Comparing it with a physical spring-mass damped oscillator having damping constant ’b’, the correct equivalence will be
1
\( L \leftrightarrow \frac{1}{b}, C \leftrightarrow \frac{1}{m}, R \leftrightarrow \frac{1}{k}\)
2
L ↔ k, C ↔ b, R ↔ m
3
L ↔ m, C ↔ k, R ↔ b
4
\(L \leftrightarrow m, C \leftrightarrow \frac{1}{k}, R \leftrightarrow b\)