Slides

Linearity & Source Transformation

12 min read

Mansoura University
Mansoura University
Faculty of Computers and Information
Department of Information Technology
First Semester
Faculty of Computers and Information
Intro to Physics · Lesson 7
Linearity & Source Transformation
Prepared by Muhammad Elsayed
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Lesson notes

Linearity & Source Transformation

Linearity is what makes every theorem work

Kirchhoff alone will always solve a circuit, but on a large network the algebra becomes punishing. The theorems that follow are shortcuts, and every one of them rests on linearity.

  • Homogeneity (scaling): multiply the input by k and the output is multiplied by the same k.
  • Additivity: the response to a sum of inputs equals the sum of the individual responses.
  • A circuit is linear only if both hold. A resistor qualifies, since v = iR is linear in both directions.
  • Power does not. p = i²R is quadratic, so no theorem in this chapter may be applied to power directly.

Using linearity directly

Scaling is a working technique, not just a property.

  • Assume a convenient output, usually io = 1 A, and work backwards to the source it would require.
  • Compare that with the real source value: the ratio is the scale factor k.
  • Multiply your assumed answer by k. This turns a ladder network into simple arithmetic.

Source transformation

Two circuits are equivalent when their terminal v-i behaviour is identical, and that is all equivalence means here.

  • A voltage source vs in series with R behaves exactly like a current source is = vs/R in parallel with the same R.
  • The current source arrow points toward the positive terminal of the voltage source it replaces.
  • Transform repeatedly, combining series and parallel elements between transforms, until the circuit collapses to a single loop.
  • The transformation is undefined when R is zero or infinite: an ideal voltage source has no series resistance to move.

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