davis testcircuit from bug #240, show achieved precision
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* switch as negative resistance oscillator
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* compare the transient simulation of this
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* switch based relaxation oscillator
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* with the analytic solution
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* show off the precision which can be achieved
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* even though switching the time-constant by 7 orders of magnitude
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I1 1 0 -100u
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C1 1 0 1n
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SW1 1 0 1 0 SWITCH1
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.MODEL SWITCH1 SW VT=2.5 VH=2.0 RON=1 ROFF=10MEG
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.option method=trap
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.control
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* two e-t/T shapes
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* one is tau1 = 10Meg*1nF = 10ms
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* rising from 0 to 100u*10Meg = 1000V
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* second is tau2 = 1Ohm*1nF = 1ns
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* falling down to 100u*1 = 100uV
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* first upper switch point t1 is
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* 4.5v = 1000v * (1 - e^-t/tau1)
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* first crossing of 0.5 point is t0
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* first crossing of 4.5 point is t1
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*
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* tr and tf, 0.5 to 4.5 and back to 0.5
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* 4.5 = 0.5 + (1000 - 0.5) * (1 - e(-tr/tau1))
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* tr = tau1 * log((1000 - 0.5)/(4.5 - 0.5))
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* 0.5 = 100u + (4.5 - 100u) * e(-tf/tau2)
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* tf = tau2 * log((4.5 - 100u)/(0.5 - 100u))
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let tau1 = 10ms
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let tau2 = 1ns
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let t0 = -tau1 * log(1 - 0.5/1000)
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let t1 = -tau1 * log(1 - 4.5/1000)
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let tr = tau1 * log((1000 - 0.5)/(1000 - 4.5))
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let tf = tau2 * log((4.5 - 100u)/(0.5 - 100u))
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let Tperiod = tr + tf
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tran 10us 300us uic
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let len = length(time)
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let gold = vector(len)
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let steps = vector(len)
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let kk = 0
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repeat $&len
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let tt = time[kk] - t0
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let tt = tt lt 0 ? tt : tt - Tperiod * floor(tt/Tperiod)
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let tt = tt + t0;
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let gold[kk] = (tt lt t1) ? 1000*(1-exp(-tt/tau1)) : (100u + (4.5-100u)*exp(-(tt-t1)/tau2))
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let steps[kk] = time[kk] - time[vecmax(kk-1, 0)]
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let kk = kk + 1
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end
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plot v(1) gold
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plot (v(1) - gold) ylimit -1mV 1mV
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* the first discharge in more detail:
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plot v(1) gold xlimit 45.095e-6 45.110e-6
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* compare the golden first discharge time
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* with the timesteps choosen in the following print
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* the last step is 1ns before the ideal switch,
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* the following is 100ps after the ideal switch
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* one can readily see the timestep truncation in action
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* when aproaching the discharge time point
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print (time - t1) steps
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.endc
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.end
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