Where is the RLC circuit time constant"2L/R" coming from?

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Discussion Overview

The discussion revolves around the origin and significance of the time constant "2L/R" in RLC circuits. Participants explore its implications for circuit behavior, particularly in relation to damping and oscillation characteristics, while questioning its physical meaning and applicability in comparison to RC and RL circuits.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants express confusion about the meaning and derivation of the time constant "2L/R" in RLC circuits, questioning its physical significance.
  • One participant describes the RLC circuit as a resonant circuit with diminishing oscillations, drawing parallels to capacitor discharge and suggesting that the time constant relates to the amplitude falling to 1/e.
  • Another participant provides a detailed derivation of the time constant from the transfer function of the RLC circuit, linking it to the damping coefficient and the exponential decay of oscillations.
  • Some participants argue that the presence of both exponential and sinusoidal terms in the RLC circuit equations complicates the definition of a time constant, suggesting it may not be well-defined in this context.
  • There is mention of the distinction between first-order circuits (RC and RL) and second-order circuits (RLC), with some participants noting that time constants are typically not used for second-order systems.
  • A later reply emphasizes that in second-order systems, the time constant can still define the slope of the envelope of decaying oscillations, relating it to settling time.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the definition and significance of the time constant in RLC circuits. There are competing views regarding its applicability and the implications of the circuit's behavior.

Contextual Notes

Some participants highlight that the RLC circuit's behavior is influenced by multiple factors, including the presence of both exponential decay and oscillatory components, which complicates the understanding of time constants compared to simpler circuits.

garylau
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Sorry
i want to ask a question about RLC circuit~
i don't understand where is this "2L/R"coming from
and also i don't know what is the function of this" time constant"(it is meaningless in physical sens?e)

in the note it states"that the time constant for reaching the steady state here..."

how did he knows this is the time constant that lead to the steady state?

thank you​
 

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Engineering news on Phys.org
This is a resonant circuit consisting of C and L together with some losses represented by R.
The oscillations gradually diminish, in an exponential manner, similar to the discharge of a capacitor. Eventually the amplitude falls almost to zero. The time constant is the period of time after which the amplitude has fallen to 1/e.
 
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Unfortunately, you didn`t show us neither the circuit diagram nor the corresponding transfer function.
Nevertheless, from the transient response one can deduce how the circuit will look like.
It is a simple RLC- lowpass.

The transfer function is H(s)=(1/sC)/(R+sL+1/sC)=1/(1+sRC+s²LC)
The poles of this function can be found by settimg the denominator to zero: 1+sRC+s²LC=0.
Result (two real poles):
s1,2=-R/2L(+-)SQRT(R²/4L²-1/LC).

Knowing that
(1) the denominator of the transfer function (frequency domain) is identical to the characteristic polynominal (time domain) and
(2) that, therefore, the the real part of the pole (-R/2L) appears in the solution of the differential equation as exp(-R/2L)t,

we can derive that the damping coefficient for the decaying oscillation is σ=R/2L.
If we compare this result with the general expression exp(-t/τ) we get τ=2L/R.
 
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LvW said:
Unfortunately, you didn`t show us neither the circuit diagram nor the corresponding transfer function.
Nevertheless, from the transient response one can deduce how the circuit will look like.
It is a simple RLC- lowpass.

The transfer function is H(s)=(1/sC)/(R+sL+1/sC)=1/(1+sRC+s²LC)
The poles of this function can be found by settimg the denominator to zero: 1+sRC+s²LC=0.
Result (two real poles):
s1,2=-R/2L(+-)SQRT(R²/4L²-1/LC).

Knowing that
(1) the denominator of the transfer function (frequency domain) is identical to the characteristic polynominal (time domain) and
(2) that, therefore, the the real part of the pole (-R/2L) appears in the solution of the differential equation as exp(-R/2L)t,

we can derive that the damping coefficient for the decaying oscillation is σ=R/2L.
If we compare this result with the general expression exp(-t/τ) we get τ=2L/R.
Oh Sorry
 

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Also for your circuit arrangement, the result of my calculation example still applies.
The reason is as follows: The current through the whole circuit (your task) has the the same form (in the time domain) as the voltage across the capacitor (my example). That means, the damping properties are identical - and hence the time constant.
 
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LvW said:
Also for your circuit arrangement, the result of my calculation example still applies.
The reason is as follows: The current through the whole circuit (your task) has the the same form (in the time domain) as the voltage across the capacitor (my example). That means, the damping properties are identical - and hence the time constant.
Oh i See

but when i try to put "2L/R" into the equation
i didn't see anything special?
there is no well-defined "amplitude" in this case?
because there are two terms
De^(Rt/2L) * Sin(omega*t)

if i try to put t=2L/R then it will become (63.4%)*D*sin(omega* 2L/R)

it seems (63.4%)* D = Amplitude of that D which the power is dissipated 50%?
 

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tech99 said:
This is a resonant circuit consisting of C and L together with some losses represented by R.
The oscillations gradually diminish, in an exponential manner, similar to the discharge of a capacitor. Eventually the amplitude falls almost to zero. The time constant is the period of time after which the amplitude has fallen to 1/e.
However i got confused here
there is no well-defined definition of amplitude in this case as the sin function terms never allow the function reaches "the new amplitude" value?
 
garylau - what now is your problem? Please, try a clear question or problem description.
 
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LvW said:
garylau - what now is your problem? Please, try a clear question or problem description.

Does RLC circuit has well-defined time constant?
In the case of RL and Rc circuit,it is clearly that there is time constant as there is only "e" terms in the equation.
but in the case of RLC circuit,the whole equation include both "e" and "sin" terms and it behaves strange.
the sin terms never allow the the function reaches its "new Amplitude" value except time=0
So it looks different from the case of LC and RC cases,is it meaningless to understand what is "time constant in RLC circuit"?
from a website
somebody said "I think that in a RLC circuit one doesn't define time constant. There has two expressions with dimensional unit: time, but that is not time constant.
T=1/((-R/2L)±SQRT((R/2L)^2-1/(LC)))"

http://forum.allaboutcircuits.com/threads/time-constant-for-rlc-circuit.877/
 
  • #10
garylau said:
Does RLC circuit has well-defined time constant?
In the case of RL and Rc circuit,it is clearly that there is time constant as there is only "e" terms in the equation.
but in the case of RLC circuit,the whole equation include both "e" and "sin" terms and it behaves strange.
the sin terms never allow the the function reaches its "new Amplitude" value except time=0
So it looks different from the case of LC and RC cases,is it meaningless to understand what is "time constant in RLC circuit"?
from a website
somebody said "I think that in a RLC circuit one doesn't define time constant. There has two expressions with dimensional unit: time, but that is not time constant.
T=1/((-R/2L)±SQRT((R/2L)^2-1/(LC)))"

http://forum.allaboutcircuits.com/threads/time-constant-for-rlc-circuit.877/
RC and RL circuits are called 'first order circuits' and their behaviour is analysed using a defined 'time constant'.
An RLC circuit is a second order circuit and its behaviour can be analysed using parameters like rise time, peak time, delay time, damping factor, natural frequency of oscillation etc. (look up step response of a second order circuit). I have not seen the concept of time constant being used directly in case of 2nd order circuits.
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cnh1995 said:
I have not seen the concept of time constant being used directly in case of 2nd order circuits.
Cnh1995 - didn`t you read my contribution in post#3 ?
In a 2nd-order sysytem the time constant defines the slope of the envelope of the decaying oscillation.
Hence, it has a direct relation to the settling time.
 

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