What are the characteristics of ideal electrical elements?

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    Electrical Elements
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Discussion Overview

The discussion focuses on the characteristics of ideal electrical elements, including voltage sources, current sources, resistors, inductors, and capacitors. Participants explore definitions, properties, and implications of these ideal components in both theoretical and practical contexts.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants describe ideal voltage and current sources, noting that an ideal voltage source has zero impedance while an ideal current source has infinite impedance.
  • Others argue that the resistance of an ideal current source is zero, while some maintain it is infinite, leading to a discussion on the definition of resistance in different contexts.
  • A participant mentions that the definition of resistance as R = V/I applies primarily in "Ohmic" situations, where the I-V curve is linear.
  • There is a discussion about the importance of source impedance when calculating equivalent circuits or time constants, with some participants recalling experiences with students overlooking this aspect.
  • Some participants express uncertainty regarding the definitions and implications of resistance in the context of ideal current sources, particularly when discussing non-Ohmic situations.
  • One participant references a personal experience with a physics book that presents R = V/I as a straightforward definition rather than as "Ohm's Law," suggesting a divergence in terminology and understanding among participants.
  • Another participant emphasizes the relevance of Norton equivalent resistance when discussing real current sources, contrasting it with the ideal case.
  • There is a mention of the relationship between voltage and current in ideal sources, with some questioning the equations used to describe these relationships.

Areas of Agreement / Disagreement

Participants express differing views on the resistance of ideal current sources, with some asserting it is infinite and others suggesting it is zero. The discussion remains unresolved regarding the implications of these definitions and their application in various contexts.

Contextual Notes

Limitations include varying interpretations of resistance in Ohmic versus non-Ohmic situations, and the potential confusion arising from different terminologies used in educational materials.

Jhenrique
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A ideial voltage source has:
v = v
i = ?
R = 0
L = ?
C = ?

ideal current source:
v = ?
i = i
R = 0
L = ?
C = ?

ideal resistor:
v = R i
i = 1/R v
R = R
L = ?
C = ?

ideal inductor:
v = L i/t
i = 1/L vt
R = 0
L = L
C = ?

ideal capacitor:
v = 1/C it
i = C v/t
R = 0
L = ?
C = C

*assuming that v, i, R, L and C, varies linearly (just for simplify...).

I'd of know the values/definition for where I setted "?".
 
Last edited:
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Ideal voltage source: I = V/Z, L = 0, C = 0
Ideal current source: V = IZ, L = 0, C = 0
Ideal resistor: C = 0, L = 0
Ideal inductor: C = 0
Ideal capacitor: L = 0

The abundance of zeros is what makes these "ideal". Although ideal inductors and capacitors have zero resistance, they have nonzero impedance.
 
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I would note that an ideal voltage source has zero impedance but the ideal current source has infinite impedance.
 
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Thanks; it didn't occur to me to mention the impedance of sources.

EDIT: Also, the resistance of a current source is not necessarily zero. You can easily multiply the current by the voltage to obtain a real, nonzero resistance in a DC circuit.
 
Nick O said:
Thanks; it didn't occur to me to mention the impedance of sources.

Yeah, normally it doesn't come up but it can matter when you wish to find equivalent circuits or calculate time constants. I always had a few students every time who would forget about the source impedance when calculating an RC time constant.
 
Nick O said:
EDIT: Also, the resistance of a current source is not necessarily zero.

But an ideal current source has resistance zero, correct!?
 
No, an ideal current source has infinite resistance.
 
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DaleSpam said:
No, an ideal current source has infinite resistance.

Has more something wrong in my first post?
 
  • #10
DaleSpam said:
No, an ideal current source has infinite resistance.

Is that really an accurate representation when we define R = V/I? This is a genuine question from a student, not a challenge from an arrogant newbie.
 
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  • #11
Nick O said:
Is that really an accurate representation when we define R = V/I? This is a genuine question from a student, not a challenge from an arrogant newbie.
Yes, it is accurate, but you have to be a little smart about R.

That definition of R only applies for "Ohmic" situations. I.e. where the I-V curve is a straight line through the origin. In those situations the resistance is the inverse slope of that line. The only time a current source has an I-V curve through the origin is when I=0, and in that case the inverse slope is infinite.

If you have a "non-Ohmic" situation (i.e. the I-V curve is not a straight line through the origin) then you have to adjust your definition of resistance. Usually you would talk about the differential resistance: dV/dI, which is infinite for a current source.

A third way that you can talk about the impedance of a current source is by considering a Norton equivalent circuit which models a real current source as an ideal current source in parallel with a source resistance. The real source becomes closer and closer to an ideal source as the source resistance becomes infinite.

So whether you are talking about Ohmic resistance at I=0, or differential resistance, or Norton equivalent resistance, an ideal current source has infinite resistance.

The chordal resistance is not infinite for I≠0, but it also not well defined, so it is rarely discussed.
 
  • #12
Thanks. The idea makes conceptual sense, and is clearly the assumption made in finding Norton equivalents. But the definition of resistance just suddenly came to mind when I made my second to last post.

My old physics book seems to be unorthodox in that it emphasizes that R=V/I is not "Ohm's Law" but rather a straightforward definition that is always true. The author used the term "Ohm's law" to refer to the observation that some materials have a linear I-V curve.

I've never personally heard an engineer or scientist use the term that way, so I may do well to forget it.
 
  • #13
Nick O said:
My old physics book seems to be unorthodox in that it emphasizes that R=V/I is not "Ohm's Law" but rather a straightforward definition that is always true.
I don't think that is standard usage, at least not for active devices, however I haven't taken a survey or anything to find out.

When talking about real current sources the resistance of the source is an important performance characteristic that any owner's manual will mention. It refers to the Norton equivalent resistance. So this real current source has a resistance of 500 MΩ and using the same meaning an ideal current source has infinite resistance.
 
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  • #14
Nick O said:
Ideal voltage source: I = V/Z, L = 0, C = 0
Ideal current source: V = IZ, L = 0, C = 0
Ideal resistor: C = 0, L = 0
Ideal inductor: C = 0
Ideal capacitor: L = 0

Actually, the current of the ideal voltage source is not computed by:
8a89f7d3622fc859d3bc910a8691b9e9.png


and the voltage of the ideal current source is not computed by:
8383fa6312eb5e0b7befb1b4172ae749.png


?

*source: http://en.wikipedia.org/wiki/Harmonic_oscillators#Equivalent_systems
 
  • #15
V=IZ is always true. You only use convoluted equations like those in systems where V and I vary with time and you cannot easily find a solution to V=IZ.

Most circuits are not harmonic oscillators, though.
 

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