A particle with restoring force proportional to displacement and resisting force proportional to velocity is subjected to a force `F sin omegat `. If the amplitude of the particle maximum for `omega=omega_(2)` then `(omega_(0)` is the angular frequency of undampled oscillations ).
A. `omega_(1)=omega_(0) ` and `omega_(2)!=omega_(0)`
B. `omega_(1)=omega_(0) ` and `omega_(2)=omega_(0)`
C. `omega_(1)!=omega_(0) ` and `omega_(2)=omega_(0)`
D. `omega_(1)!=omega_(0) ` and `omega_(2)!=omega_(0)`