The whole discipline of optical measurement techniques can be roughly subdivided into the two areas of photometry and radiometry. Whereas the central problem of photometry is the determination of optical quantities closely related to the sensitivity of the human eye (see § II.6.), radiometry deals with the measurement of energy per time ( = power, given in watts) emitted by light sources or impinging on a particular surface. Thus, the units of all radiometric quantities are based on watts (W). According to CIE regulations, symbols for radiometric quantities are denoted with the subscript “e” for “energy”. Similarly, radiometric quantities given as a function of wavelength are labeled with the prefix “spectral” and the subscript “λ” (for example spectral radiant power Φ_{λ}).
Remark: The definitions of radiometric quantities cannot be understood without a basic comprehension of differential quantities. For an intuitive understanding of these quantities, which is the main purpose of this paragraph, the differential quantities dλ, dA and dΩ can be regarded as tiny intervals or elements ∆λ, ∆A and ∆Ω of the respective quantity. As a consequence of the fact that these intervals or elements are very small, radiometric quantities can be considered constant over the range defined by dλ, dA and/or dΩ. Similarly, dΦ_{e}, dI_{e}, dL_{e} and dE_{e} can be regarded as small portions which add up to the total value of the respective quantity. In paragraph II.5., the concept of differential quantities and integral calculus is briefly explained for spectral radiometric quantities.
II.4.a. Definition of solid angle
The geometric quantity of a solid angle Ω quantifies a part of an observer’s visual field. If we imagine an observer located at point P, his full visual field can be described by a sphere of arbitrary radius r (see Fig.II.). Then, a certain part of this full visual field defines an area A on the sphere’s surface and the solid angle Ω is defined by
Ω = A / r² 
Equ. II.2 
As the area A is proportional to r², this fraction is independent of the actual choice of r.
If we want to calculate the solid angle determined by a cone, as shown in Fig.II.area A is the area of a spherical calotte. However, as the solid angle is not only defined for conical parts of the full visual field, area A can be any arbitrary shape on the sphere’s surface.
Although Ω is dimensionless, it is common to use the unit steradian (sr). The observer’s total visual field is described by the whole surface of the sphere, which is given by 4πr², and thus covers the solid angle
Ω_{total} = 4πr² / r² = 4π sr = 12.57 sr
Fig.II.6. The solid angle Ω quantifies a certain part of the visual field, seen by an observer located at P
II.4.b. Radiant power or radiant flux Φ_{e
}Radiant power Φ_{e} is defined by the total power of radiation emitted by a source (lamp, light emitting diode, etc.), transmitted through a surface or impinging upon a surface. Radiant power is measured in watts (W). The definitions of all other radiometric quantities are based on radiant power. If a light source emits uniformly in all directions, it is called an isotropic light source.
Radiant power characterizes the output of a source of electromagnetic radiation only by a single number and does not contain any information on the spectral distribution or the directional distribution of the lamp output.
Fig. II.7. The radiant power of Φ_{e} of a light source is given by its total emitted radiation.
II.4.c. Radiant intensity I_{e
}Radiant intensity I_{e} describes the radiant power of a source emitted in a certain direction. The source’s (differential) radiant power dΦ_{e} emitted in the direction of the (differential) solid angle element dΩ is given by
dΦ_{e} = I_{e} dΩ
and thus
In general, radiant intensity depends on spatial direction. The unit of radiant intensity is W/sr.
Fig. II.8. Typical directional distribution of radiant intensity for an incandescent bulb.
II.4.d. Radiance L_{e
}Radiance L_{e} describes the intensity of optical radiation emitted or reflected from a certain location on an emitting or reflecting surface in a particular direction (the CIE definition of radiance is more general. Within the frame of this tutorial, the most relevant application of radiance describing the spatial emission characteristics of a source is discussed^{ }). The radiant power dΦ_{e} emitted by a (differential) surface element dA in the direction of the (differential) solid angle element dΩ is given by
dΦ_{e} = L_{e} cos(J) dA dΩ 

Equ.II.3 
In this relation, λ is the angle between the direction of the solid angle element dΩ and the normal of the emitting or reflecting surface element dA.
From the definition of radiant intensity I_{e} it follows that the differential radiant intensity emitted by the differential area element dA in a certain direction is given by
dI_{e} = L_{e} cos(J) dA
Thus,

Equ.II.4 
whereby J is the angle between the emitting surface element dA and the direction for which I_{e} is calculated.
The unit of radiance is W/(m^{2}.sr).
II.4.e. Irradiance E_{e
}Irradiance E_{e} describes the amount of radiant power impinging upon a surface per unit area. In detail, the (differential) radiant power dΦ_{e} upon the (differential) surface element dA is given by
dΦ_{e} = E_{e} dA
Generally, the surface element can be oriented at any angle towards the direction of the beam. However, irradiance is maximised when the surface element is perpendicular to the beam:
dΦ_{e} = E_{e,normal} dA_{ normal
}
Fig. II.9 – Irradiance is defined as incident radiant power dΦ_{e} per surface area element dA.
Note that the corresponding area element dA _{normal}, which is oriented perpendicular to the incident beam, is given by
dA_{ normal} = cos(J) dA
with λ denoting the angle between the beam and the normal of dA, we get
E_{e} = E_{e,normal} cos(J) 

Equ.II.5 
The unit of irradiance is W/m².
II.4.f. Radiant exitance M_{e}_{
}Radiant exitance M_{e} quantifies the radiant power per area, emitted or reflected from a certain location on a surface. In detail, the (differential) radiant power dΦ_{e} emitted or reflected by the surface element dA is given by
dΦ_{e} = M_{e} dA
From the definition of radiance follows that the (differential) amount radiant exitance dM_{e} emitted or reflected by a certain location on a surface in the direction of the (differential) solid angle element dΩ is given by
dM_{e} = L_{e} cos(J) dΩ
and consequently

Equ.II.6 
The integration is performed over the solid angle of 2π steradian corresponding to the directions on one side of the surface and J denotes the angle between the respective direction and the surface’s normal.
The unit of radiant exitance is W/m². In some particular cases, M_{e}= E_{e }(see § II.8.a).
II.4.g. Spectral radiant power Φ_{λ}(λ), spectral radiant intensity I_{λ}(λ), spectral radiance L_{λ}(λ), spectral irradiance E_{λ}(λ), and spectral radiant exitance M_{λ}(λ)
The radiometric quantities discussed above are defined without any regard to the wavelength(s) of the quantified optical radiation. In order to quantify not only the absolute amount of these quantities but also the contribution of light from different wavelengths, the respective spectral quantities are defined.
Spectral radiant power is defined as a source’s radiant power per wavelength interval as a function of wavelength. In detail, the source’s (differential) radiant power dΦ_{e} emitted in the (differential) wavelength interval between λ and λ+dλ is given by
dΦ_{e} = Φ_{λ}(λ) dλ
This equation can be visualised geometrically (see Fig. II.10.). As dλ is infinitesimally small, spectral radiant power Φ_{λ}(λ) is approximately constant in the interval between λ and λ+dλ. Thus, the product Φ_{λ}(λ) dλ equals the area under the graph of Φ_{λ}(λ) in the interval between λ and λ+dλ. This area describes the contribution of this very wavelength interval to the total value of radiant power Φ_{e}, which is graphically represented by the total area under the graph of spectral radiant power Φ_{λ}(λ).
Mathematically, this can be expressed by the integral
The unit of spectral radiant power is W/nm or W/Å.
Fig.II.10. Relation between spectral radiant power Φ_{λ}(λ) and radiant power Φ_{e}, visualized at a hypothetical example. Radiant power emitted in the wavelength interval between λ and λ+dλ is given by the area of the shaded rectangle, which amounts to Φ_{λ}(λ) dλ. The total amount of radiant power Φ_{e} emitted over the whole spectrum is given by the area under the curve describing Φ_{λ}(λ), which is mathematically expressed by an integral.
The other spectral quantities are defined correspondingly and their units are given by the unit of the respective quantity, divided by nm or Å (seeTable VII.IV and Table VII.V). Generally, a radiant quantity can be calculated from the respective spectral quantity by integration over wavelength from λ=0 to λ=∞. However, this integration is often restricted to a certain wavelength range, which is indicated by the respective prefix. For instance, UVA irradiance is defined as
as the UVA range is defined from λ= 315 nm to λ = 400 nm.