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The equation for describing the period: = shows the period of oscillation is independent of the amplitude, though in practice the amplitude should be small. The above equation is also valid in the case when an additional constant force is being applied on the mass, i.e. the additional constant force cannot change the period of oscillation.
The period, the time for one complete oscillation, is given by the expression = =, which is a good approximation of the actual period when is small. Notice that in this approximation the period τ {\displaystyle \tau } is independent of the amplitude θ 0 {\displaystyle \theta _{0}} .
The animation has time offset so driving force is rather than ().) The Duffing equation (or Duffing oscillator), named after Georg Duffing (1861–1944), is a non-linear second-order differential equation used to model certain damped and driven oscillators.
Oscillation is the repetitive or periodic variation, typically in time, of some measure about a central value (often a point of equilibrium) or between two or more different states. Familiar examples of oscillation include a swinging pendulum and alternating current. Oscillations can be used in physics to approximate complex interactions, such ...
There is a clear analogy here between these equations and those that defined the evolution of the in-phase and out-of-phase components of oscillation in the classical case. Now, however, there is a third term w , which can be interpreted as the population difference between the excited and ground state (varying from −1 to represent completely ...
A wave can be longitudinal where the oscillations are parallel (or antiparallel) to the propagation direction, or transverse where the oscillations are perpendicular to the propagation direction. These oscillations are characterized by a periodically time-varying displacement in the parallel or perpendicular direction, and so the instantaneous ...
A parametric oscillator is a harmonic oscillator whose physical properties vary with time. The equation of such an oscillator is + + = This equation is linear in ().By assumption, the parameters and depend only on time and do not depend on the state of the oscillator.
The frequency of oscillation at x is proportional to the momentum p(x) of a classical particle of energy E n and position x. Furthermore, the square of the amplitude (determining the probability density) is inversely proportional to p ( x ) , reflecting the length of time the classical particle spends near x .