## Radiant Intensity | ECE532 Biomedical Optics ©1998 Steven L. Jacques, Scott A. Prahl Oregon Graduate Institute |

## I [W/sr] |

the radiant energy flux (or power) leaving the source, or an element of the source, in an element of solid angle containing the given direction, divided by that element of solid angle. |

The **power P [W]** from a source that is directed into a particular direction along the center of a cone encompassing a **solid angle [steradians] or [sr]** is called the **Radiant Intensity, I [W/sr]**.

The **solid angle ** describes the size of the cone of intensity radiated by the source. Consider a sphere with radius R and a cone which intersects the sphere surface to form a circle with a radius r. For the case of a narrow cone and small cone area on the sphere surface, the following approximation holds. The area of the spot is A_{circle} and the surface area of the sphere is A_{sphere}, as shown in the figure below. There are 4 steradians over the entire surface of a sphere. So the ratio A_{circle}/A_{sphere} is the fraction of the total 4 [sr] of the sphere which is encompassed by the cone.

The expressions in the above figure are correct in the limit of a small solid angle. Note that r/R equals in the limit of small . The general expression for solid angle regardless of its size is:

For an isotropic source of radiant power P [W] which radiates light equally in all directions, the radiant intensity is equal to P/(4) [W/sr].

## EXAMPLE: | ## Radiant intensity of a flashlight |

More generally, intensity refers to the limiting case of the ratio P/ for a vanishingly small cone as approaches zero:

Therefore, the local radiant intensity within an irregularly shaped non-uniform-intensity region can be mapped by interrogating each portion of the region with a small cone. One is not restricted to discussing only cones.

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