What are the characteristics of ideal electrical elements?

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SUMMARY

The discussion focuses on the characteristics of ideal electrical elements, specifically ideal voltage sources, current sources, resistors, inductors, and capacitors. An ideal voltage source has zero resistance and zero impedance, while an ideal current source possesses infinite resistance and impedance. The ideal resistor maintains a constant resistance, while both ideal inductors and capacitors have zero resistance but non-zero impedance. The conversation emphasizes the importance of understanding source impedance when calculating circuit parameters, particularly in non-Ohmic situations.

PREREQUISITES
  • Understanding of electrical circuit theory
  • Familiarity with Ohm's Law and its applications
  • Knowledge of impedance in electrical components
  • Basic concepts of linear and non-linear I-V characteristics
NEXT STEPS
  • Study the implications of source impedance in circuit analysis
  • Learn about the Norton and Thevenin equivalent circuits
  • Explore the differences between Ohmic and non-Ohmic materials
  • Investigate the behavior of real versus ideal electrical components
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Electrical engineers, physics students, and anyone involved in circuit design or analysis will benefit from this discussion, particularly those interested in the theoretical foundations of electrical components.

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 "?".
 
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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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