Why Does Current Lead Voltage in a Capacitor?

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Discussion Overview

The discussion centers on the phase relationship between voltage and current in inductors and capacitors, specifically addressing why voltage leads current in inductors and why current leads voltage in capacitors. The scope includes theoretical explanations and mathematical derivations related to these phenomena.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Exploratory

Main Points Raised

  • Some participants note that voltage leads current in inductors by 90 degrees, seeking explanations for this behavior.
  • One participant references the equation V = L di/dt to explain how the change in current generates a voltage in inductors.
  • Another participant provides a mathematical representation showing that if the current is sinusoidal, the resulting voltage is a cosine function, indicating a 90-degree phase lead.
  • Some participants argue that in inductors, the instantaneous change in voltage creates a magnetic field that inhibits current flow, resulting in a delay of 90 degrees.
  • In contrast, participants explain that in capacitors, current flows instantly, but the charge buildup on the plates does not, leading to a 90-degree delay in voltage.
  • A mathematical proof involving Laplace transforms is presented, showing how multiplying by j leads to a 90-degree phase shift in the context of capacitors.

Areas of Agreement / Disagreement

Participants generally agree on the phase relationships between voltage and current in inductors and capacitors, but the explanations for these relationships vary, indicating multiple viewpoints and reasoning approaches.

Contextual Notes

Some mathematical steps and assumptions are not fully resolved, such as the implications of applying Laplace transforms and the conditions under which the phase relationships hold true.

mohdfasieh
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HEllo ,

Can anybody answer my question;


" i know that VOltage leads in Inductor by 90 as compared to current.But i want to know WHY?"

Why voltage leads in INDUCTOR




" I know CURRENT leads in CAPACITOR as compare to VOLTAGE but i want to know why ?"

Why current leads in capacitor
 
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mohdfasieh said:
HEllo ,

Can anybody answer my question;


" i know that VOltage leads in Inductor by 90 as compared to current.But i want to know WHY?"

Why voltage leads in INDUCTOR

V = L di/dt is the basic V ~ I equation for an inductor. As you put current into an inductor, the change in current generates a voltage. A DC current into an inductor generates no net DC voltage (assuming that the parasitic DC resistance of the inductor windings is negligible).


" I know CURRENT leads in CAPACITOR as compare to VOLTAGE but i want to know why ?"

Why current leads in capacitor

I = C dV/dt is the basic V ~ I equation for a capacitor. As you push more charge onto the plates of a capacitor with the current, that changes the voltage between the plates.

These simplistic (and very useful day-to-day) equations come from Maxwell's equations in E&M. If you'd like to understand their origins better, I'd suggest that you study Maxwell's equations more, and how the simplified versions of those turn into Faraday's Law and Ampere's Law, etc. Just google some of those terms and have some fun... :biggrin:
 
In addition to what berkeman wrote:
If the current in an inductor is [tex]i(t) = I sin(\omega.t)[/tex], the voltage will be:
[tex]v(t) = L.\frac{di}{dt} = \omega.L.I cos(\omega.t)[/tex].
Since a cosine wave is a sine wave with a lead of [tex]90^o[/tex] you have your voltage lead.
 
This is my reasoning for this affect.

In an inductor the voltage will change 'instantly' however, when the voltage changes it creats a changing magnetic field. This field will inhibit the current from flowing freely. This delay in current is by 90 degrees as shown above.

In a capacitor the current will flow instantly, however the charge will not build up on capacitor's plates instantly. This delay in building the charge is what causes the 90 degree delay in voltage, as shown above.
 
A quick mathematical "proof" (which also derives the impedences of these elements) is to apply Laplace transforms to the relations expressed by the capacitor current and inductor voltage, and then substitute s = jw. Multiplying by j causes a forward rotation of 90 of the phasor, dividing by j causes a reverse rotation of the phasor by 90 degrees.

E.g.--

[tex]i(t)=C\frac{dv(t)}{dt}[/tex]

Apply Laplace, use the derivative transform, and take initial conditions to be zero:

[tex]L[i(t)]=I(s)=sC V(s)[/tex]

Set [tex]s=j\omega[/tex]:

[tex]I(j\omega)=j\omega C V(j\omega)[/tex]

Since [tex]j[/tex] is mulplying the voltage phasor the current phasor leads it by [tex]90^o[/tex]

The impedence is *by definition*:

[tex]Z_{C}(j\omega)=\frac{V(j\omega)}{I(j\omega)}=\frac{1}{j\omega C}=\frac{-j}{\omega C}[/tex]
 
Last edited:

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