How does the voltage on the inductor change over time?

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SUMMARY

The discussion focuses on analyzing the voltage across an inductor (v_{L}) in a series circuit with a resistor (R) and an alternating voltage source (v_{g} = V_{peak}sin(ωt)). Participants utilize Kirchhoff's circuit laws and the relationship v_{L} = L(dI/dt) to derive the voltage function over time. The conversation highlights the importance of using trigonometric identities and complex impedance for simplifying the analysis. Ultimately, the correct approach involves collecting terms with sine and cosine functions to solve for the phase angle (φ) and current (I_{0}).

PREREQUISITES
  • Understanding of Kirchhoff's circuit laws
  • Familiarity with inductors and resistors in AC circuits
  • Knowledge of trigonometric identities and their application
  • Basic principles of complex impedance and phasor diagrams
NEXT STEPS
  • Study the application of Kirchhoff's laws in AC circuits
  • Learn about complex impedance and how to use phasor diagrams
  • Explore trigonometric identities relevant to AC circuit analysis
  • Investigate the derivation of voltage and current relationships in RLC circuits
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Electrical engineering students, circuit designers, and anyone involved in analyzing AC circuits, particularly those working with inductors and resistors.

SimpliciusH
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Homework Statement


An alternating current is running through a serially connected inductor(L) and resistor(R). The alternating voltage causing it is:
[URL]http://upload.wikimedia.org/math/5/a/0/5a0ecaa1432c6cdce653a943b4962a21.png[/URL]

How does the voltage on the inductor change over time?

Homework Equations


Kirchhoff's cricuit laws v_{g}=v_{L}+v_{R}

The Attempt at a Solution



If I understand the text right, overall I should be searching for the v_{L}(t) function right?

Ok so I know that
v_{L}=L \frac{dI}{dt}

v_{R}=IR

therefore

\frac{dI}{dt}+\frac{R}{L}I=\frac{1}{L}\frac{dv_{g}(t)}{dt}

and this is where I get stuck. Thanks for any help!
 
Last edited by a moderator:
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It should be 1/L vg on the right-hand side of the final equation. Assume I(t) in the form of I0sin(ωt+φ) take the derivative and substitute it for dI/dt into the equation.

ehild
 
Integrate the whole thing? Like this:

I_{0}\omega cos(\omega t + \varphi)+I_{0}\frac{R}{L}\frac{sin(\omega t + \varphi)-\omega t cos(\omega t + \varphi)}{\omega^2}=\frac{1}{L}V_{peak}\frac{R}{L}\frac{sin(\omega t)-\omega t cos(\omega t)}{\omega^2}
Is this right?
 
Last edited:
vg is given: vg=Vpeaksin(ωt).
Apply the sum rule to sin(ωt+φ) and cos(ωt+φ). Collect like terms. Take into account that the equation holds for any time.

There is an easier way to solve the problem, using complex impedance or phasor diagram. Have you heard about them?

ehild
 
ehild said:
vg is given: vg=Vpeaksin(ωt).
Apply the sum rule to sin(ωt+φ) and cos(ωt+φ). Collect like terms. Take into account that the equation holds for any time.

ehild


Is this comment meant for the last version of the response?

I edited my response extensively before I noticed your reply, I now realized I should have just made a new post, since this ultimately confused me and makes communication difficult. Sorry, won't do it again.


ehild said:
There is an easier way to solve the problem, using complex impedance or phasor diagram. Have you heard about them?

ehild

I've heard of them but haven't used either before.
 
SimpliciusH said:
Integrate the whole thing? Like this:

I_{0}\omega cos(\omega t + \varphi)+I_{0}\frac{R}{L}\frac{sin(\omega t + \varphi)-\omega t cos(\omega t + \varphi)}{\omega^2}=\frac{1}{L}V_{peak}\frac{R}{L}\frac{sin(\omega t)-\omega t cos(\omega t)}{\omega^2}
Is this right?

This is just so many kinds of wrong... :(

This is what I meant to write:

I_{0}sin(\omega t + \varphi) + \frac{RI_{0}}{L}(-\frac{cos{\omega t+\varphi}{\omega}= \frac{1}{L} V_{peak} sin (\omega t)
 
Do not integrate anything. Use the sum rules:
sin(ωt+φ)=sin(ωt)cosφ+cos(ωt)sinφ and
cos(ωt+φ)=cos(ωt)cosφ-sin(ωt)sinφ.
Collect the terms with cos(ωt), and do the same with the terms containing sin(ωt).

ehild
 
ehild said:
vg is given: vg=Vpeaksin(ωt).
Apply the sum rule to sin(ωt+φ) and . Collect like terms. Take into account that the equation holds for any time.

Did you mean the trig sum rule? Edit:
ehild said:
Do not integrate anything. Use the sum rules:
sin(ωt+φ)=sin(ωt)cosφ+cos(ωt)sinφ and
cos(ωt+φ)=cos(ωt)cosφ-sin(ωt)sinφ.
Collect the terms with cos(ωt), and do the same with the terms containing sin(ωt).

ehild

It dawned on me a minute too late. :) Thank you for being so patient!
 
Last edited:
V0=Vpeak

So I go from:
LI0cos(ωt+φ)+RI0sin(ωt+φ)=V0sin(ωt)

To:

LI0cos(ωt)cosφ - LI0sin(ωt)sinφ + RI0sin(ωt)cosφ + RI0cos(ωt)sinφ = V0sin(ωt)

And collect the terms:

RI0sin(ωt)cosφ - LI0sin(ωt)sinφ - V0sin(ωt)+ RI0cos(ωt)sinφ + LI0cos(ωt)cosφ = 0 sin(ωt)(RI0cosφ - LI0sinφ - V0)+ cos(ωt)(RI0sinφ + LI0cosφ) = 0


sin(ωt)(Rcosφ - Lsinφ)+ cos(ωt)(Rsinφ + Lcosφ) = sin(ωt)V0/I0


Do I now find the φ for which this equation is true? V0 seems to be causing me problems there.
 
Last edited:
  • #10
Ok I've simplified it to:

Lcos(t\omega + \varphi)+Lsin(t\omega + \varphi)=sin(t\omega + \varphi)\frac{V_{0}}{I_{0}}
 
  • #11
You forgot that ω should be together with L.
The equation has to be true for any time t, that is for such values of t when sin(ωt)=0 (and cos (ωt)=±1) and also for such values when cos(ωt) =0 (and sin(ωt) =±1). This means that

Rsinφ + Lωcosφ=0 (*)

and

Rcosφ - Lωsinφ=V0/I0 (**)


You get φ from (*). Taking the square of both (*) and (**) and adding them up, the sinφ and cosφ terms cancel and you get an equation for I0.

ehild
 
  • #12
SimpliciusH said:
Ok I've simplified it to:

Lcos(t\omega + \varphi)+Lsin(t\omega + \varphi)=sin(t\omega + \varphi)\frac{V_{0}}{I_{0}}

That is wrong. Go back to your previous post. I answered it.

ehild
 
  • #13
ehild said:
You forgot that ω should be together with L.
The equation has to be true for any time t, that is for such values of t when sin(ωt)=0 (and cos (ωt)=±1) and also for such values when cos(ωt) =0 (and sin(ωt) =±1). This means that

Rsinφ + Lωcosφ=0 (*)

and

Rcosφ - Lωsinφ=V0/I0 (**)You get φ from (*). Taking the square of both (*) and (**) and adding them up, the sinφ and cosφ terms cancel and you get an equation for I0.

ehild
Ok I get 2*pi+pi for the value of φ

and V0/(R2+L22*cos(2*φ) for I0)
 
  • #14
I then assume put this back into the equation for VL, and derive it, I get:

V0*L/(R2+L22*cos(2*φ) times ωcos (ωt + φ)

or should I say times -ωcos (ωt) considering the value of φ.

Is this right?
 
  • #15
SimpliciusH said:
Ok I get 2*pi+pi for the value of φ

and V0/(R2+L22*cos(2*φ) for I0)

No. φ is not 2*pi + pi, and why do you write 3*pi in this way?

Rsinφ + Lωcosφ=0. What is tanφ then?

To get an expression for I0 square the equations

Rsinφ + Lωcosφ=0
and
Rcosφ - Lωsinφ=V0/I0

and add them together. Take care of the + and - signs.

ehild
 
  • #16
SimpliciusH you need to practice trigonometry.
I recommend Trigonometry by S.L. Loney to you (It's a must for you)
 

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