Today we started class of with learning about 2nd
order circuit. For second order differential equation we need additional
boundary values.
V(0)=v(0-)
Capacitor
voltage and inductor current are variables that cannot change abruptly.
Source
free series RLC Circuit: the circuit is being excited by the energy initially
stored in the capacitor and inductor.
Source
free circuits do not have voltage and current.
Series
RLC Circuit Step Response: In this lab we modeled and tested a series RLC
second order circuit by analyzing step response of a ciruit and comparing with
expected values on the dampling ration and natural frequency.
The initial value of i is given as I0 across the inductor
Pre
lab: we wrote differential equation relating Vout and Vin for the RLC circuit.
We tested step response of a
given circuit. Then we compared the measured response with expected or
calculated values based on the damping ration and natural frequency of the
circuit.
The roots
s1 and s2 are called natural frequencies, measured in
nepers per second (Np/s), because they are associated with the natural response
of the circuit; ω 0 is known as the resonant frequency or strictly
as the undamped natural frequency, expressed in radians per second (rad/s); and
α is the neper frequency or the damping factor, expressed in nepers per second.
1. If α > ω 0 , we have the
overdamped case.
2. If α = ω 0 , we have the
critically damped case.
3. If α < ω 0 , we have the
underdamped case.
The
critically damped case is the borderline between the underdamped and overdamped
cases and it decays the fastest. And overdamped case takes longer to
settle.
Damping
is the gradual loss of the initial stored energy, as evidenced by the
continuous decrease in the amplitude of the response. The damping effect is due
to the presence of resistance R. The damping factor α determines the rate at
which the response is damped.
Following is the expected graph of RLC series circuit step response. It is Underdamped circuit and
( α < ω 0 )
Following is the graph of underdamped circuit we captured on waveform.
Percent Error: we calculated 19.5% error as calculated in above few pictures. The percent error might be caused from the capacitor and inductor that we used are non ideal. The inductor has non negligible resistance.
Above is the output graph fromt the capacitor.
This graph yields a damping formula of V=0.43e^(-2340t), meaning that our experimental alpha is 2340, which is about 0.4% of our theoretical alpha value of 550000.
Summary:
Possible source of error is from our input variables, the way we measured the circuit, or maybe did wrong calculation for theoretical value.
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