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2 considered the use of optical elements to shape the mutual visibility of source points and detection points. The visibility function, renamed the impulse response or point spread function, remains of central interest under the wave model. The goal of optical sensor design is to use optical elements to program the impulse response, within physical constraints, to usefully encode target object features into detected data. This section presents wave models for the optical elements that we described using geometric models in Section 2.2. In addition, we consider diffractive optical elements, which cannot be described by ray models. As in Section 2.2, analysis of refraction and re ection at dielectric interfaces is a good starting point for optical element analysis. In analogy with Fig. 2.4, the effect of a dielectric interface on a plane wave is illustrated Fig. 4.6. A plane wave is incident on the interface in a medium of index of refraction n1. The incident eld is Ei (r) Eiexp(2piui . r). The incident wave is refracted at the interface into the second medium of index of refraction n2, and a re ected wave is returned into the rst medium. The refracted and re ected elds are Et (r) Et exp(2piut . r) and Er (r) Er exp(2pi ur . r). Boundary conditions derived from the Maxwell equations determine the relative amplitudes of these waves. The boundary conditions may be stated as follows:

At the beginning of the process of converting the dried cocoa beans into chocolate liquor, the beans are rst passed over magnets and vibrating screens to remove any unwanted debris. The beans are then roasted whole, then winnowed or passed over infrared heaters to pop the outer shell. This shell is then removed by a winnowing process which separates the non-usable shell from the nib (raw cotyledon). The roasted, de-shelled bean and/or nibs are ground to a ne particle size of about 100 120 m by different types of grinding machines, such as stone, ball, pin mills, etc.

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