---
title: "Pattern multiplication, quadrature-phase sources"
subject: "Propagation and Antenna"
chapter: 2
key: "semester_6/propagation_and_antenna:pattern-multiplication-quadrature"
source: https://www.bctengineer.com/q/semester_6/propagation_and_antenna/pattern-multiplication-quadrature
site: BCT Engineering
---

# Pattern multiplication, quadrature-phase sources

Propagation and Antenna · Chapter 2: Antenna Parameters and Arrays

- Asked in: 2080 Asoj, 2+6 marks
- Video: [Array of two isotropic point sources with opposite phase and phase quadrature | Array | Lecture 15 |](https://www.youtube.com/watch?v=ytEcjF03yPo) — Dopamine
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_6/propagation_and_antenna/pattern-multiplication-quadrature
- Whole chapter: https://www.bctengineer.com/md/semester_6/propagation_and_antenna/chapter-2

## Question

Define pattern multiplication. Derive the expression for far field pattern of an array of two isotropic point sources having equal amplitude and quadrature phase with d = λ/4.

## Short answer

Pattern multiplication: array field pattern equals element pattern times array factor of isotropic sources. For two isotropic sources with equal amplitude, quadrature phase (α=-π/2), d=λ/4: array factor E_n = cos[(π/4)(cosθ-1)]. Maximum at θ=0° (toward lagging source), null at θ=180°, forming a cardioid unidirectional end-fire pattern.

## Answer

#### Pattern multiplication

**Pattern multiplication** states that the field pattern of an array of identical, similarly oriented non-isotropic elements is the product of the pattern of one element and the pattern of the array made of isotropic point sources (array factor). Total phase = element phase + array phase.

```text
E(θ) = E_element(θ) × E_array(θ)
```

#### Two isotropic sources, equal amplitude, quadrature phase, d = λ/4

Let source 1 and source 2 lie on the x-axis, spacing *d*, with the current of source 2 **lagging** source 1 by 90° (α = −π/2). θ is measured from the axis, midpoint O as reference.

```text
             P (far field)
            /
           / θ
  1 ●-----O-----● 2  -> axis (θ = 0°)
     <- d/2 -><- d/2->
   path difference = d cosθ
```

Total phase difference at P:

```text
ψ = βd cosθ + α
βd = (2π/λ)(λ/4) = π/2 ,  α = -π/2
ψ = (π/2) cosθ - π/2 = (π/2)(cosθ - 1)
```

Adding the two fields:

```text
E = E₀ e^(-jψ/2) + E₀ e^(jψ/2) = 2E₀ cos(ψ/2)
E = 2E₀ cos[(π/4)(cosθ - 1)]
Normalised: E_n = cos[(π/4)(cosθ - 1)]
```

#### Pattern values

| θ | cosθ − 1 | E_n |
|---|---|---|
| 0° | 0 | 1.000 |
| 60° | −0.5 | 0.924 |
| 90° | −1 | 0.707 |
| 120° | −1.5 | 0.383 |
| 180° | −2 | 0 |

Maximum at θ = 0° (towards the lagging source, along the axis); null at θ = 180°. The pattern is a **cardioid** (unidirectional end fire).

```text
           90° (0.707)
          .--''--.
        .'        '.
 180° 0 1   2       > 0° (max = 1)
        '.        .'
          '--..--'
           270°
```

Physical reason: towards θ = 0°, the wave from source 1 travels λ/4 (90°) to reach source 2, which exactly cancels source 2's 90° lag, so the fields add. Towards θ = 180°, the travel delay and current lag add to 180°, so the fields cancel. If source 2 leads instead (α = +π/2), the cardioid points to θ = 180°.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. Pattern multiplication is
   A. E = element pattern × array pattern, with phases added
   B. Element pattern + array pattern
   C. Array pattern squared
   D. Element pattern ÷ array pattern
   Answer: A. It applies to identical similarly oriented elements. (Key point: Definition)

2. For d = λ/4 and α = -π/2, ψ equals
   A. (π/2)(cosθ + 1)
   B. (π/2)(cosθ - 1)
   C. π cosθ
   D. (π/4) cosθ
   Answer: B. βd = π/2 and α = -π/2. (Key point: Phase difference)

3. Where is the null of E_n = cos[(π/4)(cosθ - 1)]?
   A. θ = 0°
   B. θ = 90°
   C. θ = 180°
   D. θ = 60°
   Answer: C. At 180° the argument is -π/2. (Key point: Null direction)

4. Why is the field maximum toward θ = 0°?
   A. The λ/4 travel delay cancels source 2's 90° lag, so fields add
   B. Because the sources are isotropic
   C. Because the delay doubles the lag
   D. Because the amplitudes differ
   Answer: A. At 180° the delay and lag add to 180° and cancel. (Key point: Physical reason)

## Related in Propagation and Antenna

- [Two isotropic sources, equal amplitude, opposite phase](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Atwo-sources-opposite-phase) — Propagation and Antenna, chapter 2, asked 3×
- [Two isotropic sources, same and opposite phase](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Atwo-sources-same-and-opposite-phase) — Propagation and Antenna, chapter 2, asked 3×
- [Opposite-phase two-source array maxima and minima](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Atwo-sources-opposite-maxima-minima) — Propagation and Antenna, chapter 2, asked 2×
- [Pattern lobes and 180° out-of-phase array](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Alobes-importance-opposite-phase-array) — Propagation and Antenna, chapter 2
- [Two-element array and end fire pattern](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Atwo-isotropic-endfire-pattern) — Propagation and Antenna, chapter 2
- [Pattern multiplication for two short dipoles](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Apattern-multiplication-short-dipoles) — Propagation and Antenna, chapter 2
