# 1.7 Basic Photometric Quantities

One of the central problems of optical measurements is the quantification of light sources and lighting conditions in numbers directly related to the perception of the human eye. This discipline is called “photometry” and its significance leads to the use of separate physical quantities that differ from the respective radiometric quantities in only one respect: Whereas radiometric quantities simply represent a total sum of radiation power at various wavelengths and do not account for the fact that the human eye’s sensitivity to optical radiation depends on wavelength, the photometric quantities represent a weighted sum with the weighting factor being defined by either the photopic or scotopic spectral luminous efficiency function. Thus, the numerical value of photometric quantities directly relates to the impression of “brightness”. Photometric quantities are distinguished from radiometric quantities by the index “v” for “visual”. Furthermore, photometric quantities relating to scotopic vision are denoted by an additional prime, for example Φv’. The following explanations are given for the case of photopic vision, which describes the eye’s sensitivity under daylight conditions and are therefore very significant for the vast majority of lighting situations (photopic vision takes place when the eye is ad /en-us/service-and-support/knowledge-base/basics-light-measurement/appendix/?stage=Stage ted to luminance levels of at least several candelas per square meters, scotopic vision takes place when the eye is adapted to luminance levels below some hundredths of a candela per square meter. For mesopic vision, which is between the photopic and scotopic range, no spectral luminous efficiency function has been defined yet). However, the respective relations for scotopic vision can be easily derived by replacing V(λ) with V'(λ) and K_{m} (= 683 lm/W) with K'_{m} (= 1700 lm/W).

Since the definition of photometric quantities closely follows the corresponding definitions of radiometric quantities, the corresponding equations hold true – the index “e” only has to be replaced by the index “v”. Thus, not all relations are repeated. Instead, a more general formulation of all relevant relations is given in the Appendix.

Measuring instruments for these applications are often called photometers or in the case of illuminance measurement luxmeters as well as spectral photometers or respectively spectral luxmeters.

### The following sections give information on:

### Luminous flux Φv

Luminous flux Φv is the basic photometric quantity and describes the total amount of electromagnetic radiation emitted by a source, spectrally weighted with the human eye’s spectral luminous efficiency function V(λ). Luminous flux is the photometric counterpart to radiant power. The luminous flux is given in lumen (lm). At 555 nm where the human eye has its maximum sensitivity, a radiant power of 1 W corresponds to a luminous flux of 683 lm. In other words, a monochromatic source emitting 1 W at 555 nm has a luminous flux of exactly 683 lm. The value of 683 lm/W is abbreviated as Km (the value of Km = 683 lm/W is given for photopic vision. For scotopic vision, K_{m}' = 1700 lm/W has to be used). However, a monochromatic light source emitting the same radiant power at 650 nm, where the human eye is far less sensitive and V(λ) = 0.107, has a luminous flux of 0.107 × 683 lm = 73.1 lm. For a more detailed explanation of the conversion of radiometric to photometric quantities, see paragraph Conversion between radiometric and photometric quantities.

### Luminous intensity Iv

Luminous intensity Iv quantifies the luminous flux emitted by a source in a certain direction. It is therefore the photometric counterpart of the “radiant intensity (I_{e})”, which is a radiometric quantity. In detail, the source’s (differential) luminous flux dΦ_{v} emitted in the direction of the (differential) solid angle element dΩ is given by

dΦ_{v}= I_{v}× dΩ

and thus

Φ_{v}=∫ I_{v}dΩ4π

The luminous intensity is given in lumen per steradian (lm/sr). 1 lm/sr is referred to as **“candela” (cd):**

1 cd = 1 lm/sr

### Luminance Lv

Luminance L_{v} describes the measurable photometric brightness of a certain location on a reflecting or emitting surface when viewed from a certain direction. It describes the luminous flux emitted or reflected from a certain location on an emitting or reflecting surface in a particular direction (the CIE definition of luminance is more general. This tutorial discusses the most relevant application of luminance describing the spatial emission characteristics of a source is discussed). In detail, the (differential) luminous flux dΦ_{v} emitted by a (differential) surface element dA in the direction of the (differential) solid angle element dΩ is given by

dΦ_{v}= L_{v}cos(Θ) × dA × dΩ

with Θ denoting the angle between the direction of the solid angle element dΩ and the normal of the emitting or reflecting surface element dA.

The unit of luminance is

1 lm m^{-2}sr^{-1}= 1 cd m^{-2}

### Illuminance Ev

Illuminance E_{v} describes the luminous flux per area impinging upon a certain location of an irradiated surface. In detail, the (differential) luminous flux dΦ_{v} upon the (differential) surface element dA is given by

dΦ_{v}= E_{v}× dA

Generally, the surface element can be oriented at any angle towards the direction of the beam. Similar to the respective relation for irradiance, the illuminance E_{v} upon a surface with arbitrary orientation is related to illuminance E_{v, normal} upon a surface perpendicular to the beam by

E_{v }= E_{v, normal}cos(ϑ)

with ϑ denoting the angle between the beam and the surface’s normal. The unit of illuminance is **lux (lx)**.

1 lx = 1 lm m^{-2}

### Luminous exitance Mv

Luminous exitance M_{v} quantifies the luminous flux emitted or reflected from a certain location on a surface per area. In detail, the (differential) luminous flux dΦ_{v} emitted or reflected by the surface element dA is given by

dΦ_{v }= M_{v}× dA

The unit of luminous exitance is 1 **lm m ^{-2}**, which is the same as the unit for illuminance. However, the abbreviation lux is

**not**used for luminous exitance.

### Conversion between radiometric and photometric quantities

**Monochromatic radiation**

In the case of monochromatic radiation at a certain wavelength λ, a radiometric quantity X_{e} is simply transformed to its photometric counterpart X_{v} by multiplication with the respective spectral luminous efficiency V(λ) and by the factor K_{m} = 683 lm/W. Thus,

X_{v}= X_{e}× V(λ) × 683 lm/W

with X denoting one of the quantities Φ, I, L, or E.

Example: An LED (light emitting diode) emitsnearly monochromatic radiation at λ = 670 nm, where V(λ) = 0.032. Its radiant power amounts to 5 mW. Thus, its luminous flux equals

Φ_{v}= Φ_{e}× V(λ) × 683 lm/W = 0.109 lm = 109 mlm

Since V(λ) changes very rapidly in this spectral region (by a factor of 2 within a wavelength interval of 10 nm), LED light output should not be considered monochromatic in order to ensure accurate results. However, using the relations for monochromatic sources still results in an approximate value for the LED’s luminous flux which might be sufficient in many cases.

**Polychromatic radiation**

If a source emits polychromatic light described by the spectral radiant power Φ_{λ}(λ), its luminous flux can be calculated by spectral weighting of Φ_{λ}(λ) with the human eye’s spectral luminous efficiency function V(λ), integration over wavelength and multiplication with K_{m} = 683 lm/W, so

Φ_{v}= K_{m}×∫ Φ_{λ}(λ) × V(λ)dλλ

In general, a photometric quantity X_{v} is calculated from its spectral radiometric counterpart X_{λ}(λ) through the relation

X_{v}= K_{m}×∫ X_{λ}(λ) × V(λ)dλλ

with X denoting one of the quantities Φ, I, L, or E.