Skip to main content
Speclore

Optical Distance Law

Reference data and engineering information about optical distance law for miscellaneous applications.

opticaldistancelaw

Overview

Engineering reference data for Optical Distance Law in miscellaneous.

Key Formulas

Unit Conversion

y=xky = x \cdot k

Multiply by conversion factor.

Linear Interpolation

y=y1+(xx1)(y2y1)x2x1y = y_1 + \frac{(x - x_1)(y_2 - y_1)}{x_2 - x_1}

Estimate between two known points.

Percentage

p=partwhole×100%p = \frac{\text{part}}{\text{whole}} \times 100\%

Part as fraction of whole.

Variables

SymbolDescriptionUnit
xxInput value
yyOutput value
kkConversion factor

Practical Example

Illumination at Different Distances

Consider a lamp with a luminous flux of 10000 lumens (lm).

Calculation at distance 1 (d₁ = 2 m): Using the basic formula:

E1=Φd12=10000lm(2m)2=2500luxE_1 = \frac{\Phi}{d_1^2} = \frac{10000 \, \text{lm}}{(2 \, \text{m})^2} = 2500 \, \text{lux}

Calculation at distance 2 (d₂ = 5 m): Using the ratio form of the law:

E2=E1d12d22=2500lux(2m)2(5m)2=400luxE_2 = E_1 \cdot \frac{d_1^2}{d_2^2} = 2500 \, \text{lux} \cdot \frac{(2 \, \text{m})^2}{(5 \, \text{m})^2} = 400 \, \text{lux}

This example demonstrates the significant reduction in illumination intensity over a relatively short distance due to the inverse-square relationship.

Cosine Law of Illumination

When the surface is not perpendicular to the direction of the light, the cosine law (also known as Lambert's cosine law) provides a more general relationship.

The illumination intensity EE on a surface is given by:

E=Φd2cos(θ)E = \frac{\Phi}{d^2} \cos(\theta)

Where:

  • θ\theta (theta) is the angle between the light ray and the normal (perpendicular line) to the illuminated surface.

Implication: Maximum illumination occurs when the light strikes the surface perpendicularly (θ=0\theta = 0^\circ, cos(0)=1\cos(0^\circ)=1). As the angle of incidence increases, the illumination decreases.

Key Relationship

The core principle is that illumination EE is inversely proportional to the square of the distance dd from the point light source. This is captured in the relationship:

E1d2E \propto \frac{1}{d^2}

This fundamental law is critical for lighting design, photography, and optical engineering.

References