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Lesson Alternating current · Math for AC

Vectors and Pythagoras

A vector has magnitude (how much) and direction (which way). When two forces, displacements, or electrical quantities act at right angles, you combine them with the Pythagorean theorem: a² + b² = c². That is not classroom trivia—it is how you find total voltage drop, resultant current, and later impedance without treating AC like simple DC addition.

1

Scalar vs vector

A scalar is a number only: 120 V magnitude with no direction, 10 A, 50 ft of wire. A vector adds direction: 120 V leading current by 30°, a force northeast at 50 lb, a displacement 3 ft east plus 4 ft north.

In AC, voltage and current are often vectors because they can point different ways on a time diagram (phase). Even before phase, any two effects at right angles combine with Pythagoras—not by straight addition.

2

Pythagorean theorem

In any right triangle:

a² + b² = c²

where c is the hypotenuse (the longest side, opposite the 90° corner) and a and b are the two shorter sides.

Example. a = 3, b = 4 c² = 3² + 4² = 9 + 16 = 25 c = √25 = 5

The classic 3-4-5 triangle appears constantly in layout and in vector sketches. Scale it: 6-8-10, 9-12-15—same shape.

3

Finding the resultant of perpendicular vectors

To add two vectors that are 90° apart:

  1. Draw one vector along the x-axis (horizontal).
  2. Draw the second from the tip of the first, vertical.
  3. The resultant runs from the start of the first to the end of the second—the hypotenuse.

Magnitude: R = √(A² + B²) Direction: θ = tan⁻¹(B / A) from the horizontal reference.

Example. Horizontal component 6 V, vertical component 8 V. R = √(36 + 64) = √100 = 10 V θ = tan⁻¹(8/6) ≈ 53.1°

4

When vectors are not perpendicular

Head-to-tail method still works: slide the second vector so its tail touches the first vector's head. The resultant is the closing line. If the angle is not 90°, use trigonometry (law of cosines) or a scale drawing. In this course, most field examples start with right-angle combinations—the Pythagorean case.

5

Vector subtraction

Subtracting vector B from A is the same as adding −B (same length, opposite direction). In AC troubleshooting you sometimes compare before and after a change: the difference between two phasors tells you what a capacitor or inductor added to the circuit.

6

Practical electrical preview

Imagine two voltage drops in a branch: one purely resistive (in phase with current) and one purely reactive (90° shifted)—you will study those parts later. Their total drop is not 6 V + 8 V = 14 V if they are orthogonal; it is √(6² + 8²) = 10 V. Treating AC drops like DC addition is one of the most expensive mistakes in the trade.

7

Units and scale

Vectors carry the same units as the quantity: volts, amperes, ohms (as impedance magnitude), or feet for mechanical analogies. When adding, both components must use consistent units and the same reference direction. A sketch at 1 cm = 2 V is fine on paper; on site, use the same ratio on every leg.

8

Resolving a vector into components

Any vector can be split into two perpendicular components—often horizontal (x) and vertical (y). If magnitude is M and angle from horizontal is θ:

  • Horizontal component: M × cos θ
  • Vertical component: M × sin θ

This is the reverse of adding components. A 10 V vector at 53.1° has horizontal 6 V and vertical 8 V—matching our earlier example. In AC, you will resolve impedance and voltage into real and reactive parts, then recombine with Pythagoras for totals.

9

Mechanical analogy that sticks

Push a cart 3 ft east, then 4 ft north. You did not travel 7 ft from start—you are 5 ft away in a straight line northeast. Walk the same path with a tape: the diagonal is the resultant displacement. Electrical vectors obey the same geometry; only the units change from feet to volts or amperes.

10

Checking your work

  • Resultant must be longer than either perpendicular leg alone (unless one leg is zero).
  • For equal legs at 90°, resultant = leg × √2 (45° case).
  • If R seems smaller than one component, you probably subtracted when you should have combined orthogonal parts with Pythagoras.
  • Dimensions must match: never add volts directly to amperes—vectors combine only when they represent the same kind of quantity in the same diagram.
11

Field case

Situation. A motor branch shows 6 V drop measured in phase with current on the feeder and 8 V drop on a reactive part of the same path (measured 90° shifted on a scope demo during training). A helper adds 6 + 8 and reports 14 V total drop—then wonders why the math disagrees with the phasor diagram.

Correct approach. Perpendicular components: Total = √(6² + 8²) = 10 V

Applied lesson. Orthogonal components combine with Pythagoras. Parallel readings on a multimeter alone cannot always reveal the 90° split—you need to know what kind of drop each measurement represents. This course builds that distinction lesson by lesson.

In the field

Symptom

Total voltage, current, or drop “too small” vs sum of parts

Where to look

Whether components are in phase or 90° apart

Likely causes

  1. Added magnitudes instead of vector sum
  2. wrong reference angle

What to measure

  1. Each component relative to a common reference (often current)

What not to do

  • Add RMS readings blindly when phase differs

Checklist

  • I distinguish scalar magnitude from vector (magnitude + direction)
  • I apply a² + b² = c² for perpendicular components
  • I can find resultant magnitude and angle with tan⁻¹
  • I sketch head-to-tail before calculating
  • I recognize the 3-4-5 and 6-8-10 triangles
  • I do not add orthogonal AC effects arithmetically

Common mistakes

Symptom Typical cause Action
Total less than largest single reading Used subtraction or wrong sign Re-sketch head-to-tail
Total = simple sum of 6 and 8 Ignored 90° phase Use √(A² + B²)
Angle off by 90° Swapped opposite and adjacent for tan Label horizontal vs vertical legs
Absurd hypotenuse Forgot square root at end c = √(a² + b²), not a² + b²