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NIU PHYS 600 - Van der Pol

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Van der PolConvergenceEquivalent CircuitNegative ResistanceSteady StateFrequency LockingRelaxation OscillatorLimit CycleVan der PolVan der PolConvergenceConvergenceThe damped driven oscillator The damped driven oscillator has both transient and has both transient and steady-state behavior.steady-state behavior.•Transient dies outTransient dies out•Converges to steady stateConverges to steady stateqqtfqqqcos220 22222022022042arctancoscostftaeqtEquivalent CircuitEquivalent CircuitOscillators can be simulated Oscillators can be simulated by RLC circuits.by RLC circuits.•Inductance as massInductance as mass•Resistance as dampingResistance as damping•Capacitance as inverse Capacitance as inverse spring constantspring constantvinvCLRCqvvCout22dtqdLdtdiLvLdtdqRRivR0RCLinvvvvtVvLCdtdvLRdtvdsin10222LR2LC120Negative ResistanceNegative ResistanceDevices can exhibit negative Devices can exhibit negative resistance.resistance.•Negative slope current vs. Negative slope current vs. voltagevoltage•Examples: tunnel diode, Examples: tunnel diode, vacuum tubevacuum tubeThese were described by Van These were described by Van der Pol.der Pol.R. V. Jones, Harvard University tVvvvdtddtvdsin0220322Steady StateSteady StateAssume an oscillating Assume an oscillating solution.solution.•Time varying amplitude Time varying amplitude VV•Slow time variationSlow time variationThe equation for V follows The equation for V follows from substitution and from substitution and approximation.approximation.The steady state is based on The steady state is based on the relative damping terms.the relative damping terms...)(21ccetVvti 02432121022220ViVViViV342VFrequency LockingFrequency LockingThe amplitude term can be The amplitude term can be separated.separated.•Two coupled equationsTwo coupled equations•Detuning term Detuning term dd•Locking coefficient Locking coefficient llThe detuning is roughly the The detuning is roughly the frequency difference.frequency difference.For small driving force the For small driving force the locking coefficient depends locking coefficient depends on the relative damping.on the relative damping.)()(tieVtV sin22cos24321022002VVVVVV sinld83200VVVl Relaxation OscillatorRelaxation OscillatorThe Van der Pol oscillator The Van der Pol oscillator shows slow charge build up shows slow charge build up followed by a sudden followed by a sudden discharge.discharge.The oscillations are self The oscillations are self sustaining, even without a sustaining, even without a driving force.driving force.Wolfram Mathworld 012 yyyyLimit CycleLimit CycleThe phase portraits show The phase portraits show convergence to a steady convergence to a steady state.state.This is called a This is called a limit cyclelimit


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NIU PHYS 600 - Van der Pol

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