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At this point, you have objects with a diffuse texture and an environment map applied on top of it. This is already a huge improvement over objects without environment maps at all. However, when I implemented this technique with the plants, the leaves were not shiny enough. They were a bit reflective, but they didn t have shiny spots that stood out, which is the effect I originally set out to find. The reason for this is that the environment map is applied uniformly to the whole object. Some places in the environment map will be brighter than others, but the surface of the object is equally reflective everywhere. Look at the objects around you, especially if there are any wet ones, and you ll quickly see that some parts are more reflective than others. For example, dry spots are not very reflective, and the fleshy parts of a leaf are much more reflective than the stem. Before we go any further, let s look at the equation that determines how you re rendering each pixel of a model with the environment map technique so far: C=L T+E Here, C is the final pixel color, L is all the incident light colors, T is the value of the texture at that point, and E is the color contribution from the environment map reflected at that point. You can implement different amounts of reflection with a specular mask: a grayscale texture that is white where the object is fully reflective and is black where it doesn t reflect at all. Intermediate gray values indicate how shiny it is at each spot. All you have

Most mechanical properties are structure-sensitive; that is, they are affected by changes in either the lattice structure or the microstructure. However, modulus of elasticity is one property that is structure-insensitive. For example, ductility and toughness of any material (regardless of whether it is a pure element such as copper, a simple alloy such as AISI 1080 steel, or a complex alloy such as a cobalt-base superalloy) vary with grain size, amount of cold work if any, or the microstructure if heat-treated. The modulus of elasticity of any material is the same regardless of grain size, amount of cold work, or microstructure.

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

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SERIN ipin,17197,[WAIT(" CHAN"), dec1 chan, STR msg\19\10] debug STR msg pause 200 serout opin,17197,[STR msg\19] branch chan-1,[st1,st2,st3,st4] st1: xout mpin,zpin,[houseA\unit1] xout mpin,zpin,[houseA\uniton] pause 15000 xout mpin,zpin,[houseA\unitoff] pause 20000 low tele goto init st2: xout mpin,zpin,[houseB\unit1] xout mpin,zpin,[houseB\uniton] pause 15000 xout mpin,zpin,[houseB\unitoff] pause 20000 low tele goto init st3: xout mpin,zpin,[houseC\unit1] xout mpin,zpin,[houseC\uniton] pause 15000 xout mpin,zpin,[houseC\unitoff] pause 20000 low tele goto init st4: xout mpin,zpin,[houseD\unit1] xout mpin,zpin,[houseD\uniton] pause 15000 xout mpin,zpin,[houseD\unitoff] pause 20000 low tele goto init

Mechanical properties are discussed individually in the sections that follow. Several new quantitative relationships for the properties are presented here which make it possible to understand the mechanical properties to a depth that is not possible by means of the conventional tabular listings, where the properties of each material are listed separately.

Hardness is used more frequently than any other of the mechanical properties by the design engineer to specify the final condition of a structural part. This is due in part to the fact that hardness tests are the least expensive in time and money to conduct. The test can be performed on a finished part without the need to machine a special test specimen. In other words, a hardness test may be a nondestructive test in that it can be performed on the actual part without affecting its service function. Hardness is frequently defined as a measure of the ability of a material to resist plastic deformation or penetration by an indenter having a spherical or conical end. At the present time, hardness is more a technological property of a material than it is a scientific or engineering property. In a sense, hardness tests are practical shop tests rather than basic scientific tests. All the hardness scales in use today give relative values rather than absolute ones. Even though some hardness scales, such as the Brinell, have units of stress (kg/mm2) associated with them, they are not absolute scales because a given piece of material (such as a 2-in cube of brass) will have significantly different Brinell hardness numbers depending on whether a 500-kg or a 3000-kg load is applied to the indenter.

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