A particle of mass (m) is attached to a spring (of spring constant k) and has a narural angular frequency omega_(0). An external force `R(t)` proportional to cos omegat(omega!=omega)(0) is applied to the oscillator. The time displacement of the oscillator will be proprtional to.

A particle of mass (m) is attached to a spring (of spring constant k) and has a natural angular frequency omega_(0) . An external force R(t) proportional to cos omegat(omega!=omega_0) is applied to the oscillator. The time displacement of the oscillator will be proportional to.

A particle of mass (m) is attached to a spring (of spring constant k) and has a natural angular frequency omega_(0) . An external force F(t) proportional to cos omegat (omega!=omega_(0)) is applied to the oscillator. The time displacement of the oscillator will be proportional to.

A particle of mass m is attached to a spring of spring constant .k. and has a natural frequency omega_(0) . An external force F(t) proportional to cos omega t(omega != omega_(0)) is applied to the oscillator. The maximum displacement of the oscillator will be proportional to

For a body of mass m attached to the spring, the spring factor is given by (omega , the angular frequency)

A particle of mass m is attached to three identical springs of spring constant k as shwon in figure. The time period of vertical oscillation of the particle is