Why Does a Current Source Have Internal Resistance in Parallel?

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Discussion Overview

The discussion revolves around the modeling of current sources in electrical circuits, specifically addressing why a current source is represented with internal resistance in parallel rather than in series. The scope includes theoretical aspects of circuit analysis and the implications of Thevenin and Norton theorems.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • One participant questions the rationale behind modeling a current source with internal resistance in parallel, seeking clarification on the appropriateness of this approach.
  • Another participant references Thevenin and Norton theorems, suggesting that any network can be characterized by either an emf in series or a current source in parallel with a resistance, though practical applications may vary.
  • A different viewpoint asserts that an ideal current source is defined as having zero ohms of source resistance, and when paralleled with a resistor, it behaves like a voltage source in series with that resistor, leading to equivalent voltage calculations.
  • Another participant challenges the previous definitions, stating that an ideal current source has infinite resistance and that real current sources possess some conductance, allowing them to be represented as a combination of ideal sources and resistors.
  • This participant also explains the operational differences between current and voltage sources in practical terms, noting how they appear in circuit configurations.

Areas of Agreement / Disagreement

The discussion contains multiple competing views regarding the definitions and characteristics of ideal and real current sources, as well as their modeling in circuits. There is no consensus on the best approach to represent current sources.

Contextual Notes

Participants express varying definitions of ideal and real current sources, highlighting assumptions about resistance and conductance that may not be universally accepted. The discussion also reflects differing interpretations of Thevenin and Norton theorems.

electroboy12
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hello.. this is my first post..forgive me if my question is wrong.. Why does a current source is modeled in such a way that it has its internal resistance in parallel ? Why can't it have its internal resistance in series ? The question may seem awkward , but please answer me.. thanks in advance..
 
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This may not be intuitive but Thevenin and Norton theorems tell you that any network of emf / current sources and resistances can be characterised by either an emf in series with or a current source in parallel with an appropriate resistance. That is not to say that it would be the best way to produce either, in practice! You could be making a lot of smoke if you chose the inappropriate one to use.
 
A current source is defined as, well, a source of current that has zero ohms source resistance. Electrically, this current source, when it is paralleled with a resistor, behaves identically to a voltage source that is in series with that same resistor. The amount of equivalent voltage is the product of the current (source) times the paralleled resistor.
 
Not a correct definition for an Ideal Source. An ideal current source has infinite resistance - in the same way that an ideal voltage source has zero resistance.

A real current source will have some Conductance (i.e. not infinite resistance) so it can actually be replaced by a suitable combination of ideal voltage or current source with a resistor.

A current source will provide just enough volts to drive the required current into the load and a voltage source will provide just enough current to develop the required voltage across the load. In practical terms this means that a current source (Anode, for instance) looks like a high resistance whilst a voltage source (Transistor emitter, for instance) looks like a low resistance.
 

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