Electronic – Instantaneous DC output using Laplace transform

dclaplace transform

I am testing a feedback system in which a feedback signal from sensor is applied to a correction network and then compared with threshold values.

I need some clue on how to get around this task, I will be applying DC voltage to the network and will compare its output obtained with the one I calculated theoretically. Here is the transfer function of the network with a natural frequency of 90Hz

$$H(s)=\dfrac{1+0.145s+0.0019s^2}{1+\dfrac{0.8}{150 }s+\dfrac{1}{150²}s²}×\dfrac{1}{1+0.0012s}×\dfrac{1}{1+0.008s}$$

I calculated the output of the network by finding its inverse Laplace with step function as its input. The issue is that the output voltage obtained from solving this is a non-linear function hence changes it at every instant so how am I supposed to test the output for a particular DC input?

Any ideas?

Here is the step response I plotted using Matlab

enter image description here

Best Answer

What you have are: two 1st order lag terms, and a 2nd order underdamped term with the slight complication of a 2nd order numerator.

The general ROT is that the settling time for a 1st order lag is \$4\tau\$ where \$\tau\$ is the time constant (\$\tau\$ is the coefficient of \$s\$ in the general term: \$1/(1+\tau s)\$). The settling time for a 2nd order denominator term is given by: \$4/(\zeta \times \omega_n)\$ where \$\zeta\$ is the damping coefficient and \$\omega_n\$ is the natural frequency.

One standard form for the 2nd order denominator is: \$1 + 2(\zeta/\omega_n)s + s^2/\omega_n^2\$

In your case \$\omega_n=150\$ rad/sec and \$\zeta=0.4\$, hence the settling time for this term is \$4/(0.4 \times 150) = 0.067 = 67\$ms. Note, for this particular application we can ignore the 2nd order numerator as it only has a small effect on the transient generated by the denominator.

The two 1st order terms give settling times: \$4 \times 1.2 = 4.8\$ms, and \$4 \times 8 = 32\$ms. The longest settling time is thus \$67\$ms, after which all the transients may be considered spent.

The steady-state gain (or 'DC gain') of the sensor is unity. This can determined by setting \$s = 0\$ in the TF.

Here's a useful plotting tool for time domain and frequency domain responses from Laplace TFs:

http://sim.okawa-denshi.jp/en/dtool.php

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