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Sub Command1_Click () Static q(25) Static p(25) Picture1.Cls 'Set variables p(1) = .9 w11 = .4 w12 = 1 w22 = .6 q(1) = 1 - p(1) 'Calculate p and q values For i = 2 To 25 wbar = p(i - 1) ^ 2 * w11 + 2 * p(i - 1) * q(i - 1) * w12 + q(i - 1) ^ 2 * w22 q(i) = (q(i - 1) ^ 2 * w22 + p(i - 1) * q(i - 1) * w12) / wbar p(i) = 1 - q(i) Next i 'Draw axes and grid Picture1.Scale (-1, 1.1)-(26, -.1) Picture1.Line (0, 0)-(0, 1) For i = 0 To 10 Picture1.Line (0, .1 * i)-(25, .1 * i) Next i For i = 5 To 25 Step 5 Picture1.Line (i, 0)-(i, 1) Next i 'Draw q values Picture1.DrawWidth = 5 For i = 1 To 25 Picture1.PSet (i, q(i)) Next i End Sub Figure 1 A Microsoft Visual Basic computer program for the simulation of heterozygote advantage. The rst statement

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The materials of the bearing also influence the performance of the system that utilizes aerostatic bearings According to Slocum [1], the main properties that are desirable to be considered in selecting aerostatic bearings material are as follows: Corrosion resistance Materials whose electrochemical potential varies by more than 025 V are not recommended Thermal expansion It is wise to match thermal expansion rates as far as is practical If precise machining is not possible, it is necessary to investigate the consequences and to adjust clearances if necessary Aerostatic bearing bush materials Bronzes are highly recommended Lead bronze is corrosion resistant and has good anti-seizure properties These materials can be easily rectified when damaged and may be used as relatively thin shells shrunk fitted into body bores

0 r 0

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indicates that the program is run by clicking a command button. Twenty- ve values of q and p are calculated and stored for printing. The program also prints a grid of lines at increments of q 0.1 and generations 5.

r 0

The McGraw Hill Companies, 2001

is characterized by the fact that the relative permeability of magnetic materials is not a constant, but is a function of the magnetic eld intensity In effect, all magnetic materials exhibit a phenomenon called saturation, whereby the ux density increases in proportion to the eld intensity until it cannot do so any longer Figure 1630 illustrates the general behavior of all magnetic materials You will note that since the B-H curve shown in the gure is nonlinear, the value of (which is the slope of the curve) depends on the intensity of the magnetic eld To understand the reasons for the saturation of a magnetic material, we need to brie y review the mechanism of magnetization The basic idea behind magnetic materials is that the spin of electrons constitutes motion of charge, and therefore

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magnetization Br To bring the ux density to zero, we must further decrease the mmf (ie, produce a negative current), until the eld intensity reaches the value H0 (point on the curve) As the mmf is made more negative, the curve eventually reaches the point If the excitation current to the coil is now increased, the magnetization curve will follow the path = = = , eventually returning to the original point in the B-H plane, but via a different path The result of this process, by which an excess magnetomotive force is required to magnetize or demagnetize the material, is a net energy loss It is dif cult to evaluate this loss exactly; however, it can be shown that it is related to the area between the curves of Figure 1632 There are experimental techniques that enable the approximate measurement of these losses Figures 1633(a) (c) depict magnetization curves for three very common ferromagnetic materials: cast iron, cast steel, and sheet steel These curves will be useful in solving some of the homework problems

the number of generations is twenty ve. The program calculates the mean tness of the population, wbar, as p2(w11) 2pq(w12) q2(w22); it then calculates the new allelic frequencies after one generation of se1.0 0.9 0.8 0.7 0.6

Advantages and limitations of journal bearings [9, 38]

Flux density (webers per square meter) Flux density (webers per square meter)

B (T)

lection (the new proportion of aa homozygotes plus half the proportion of heterozygotes). The program then repeats this process twenty- ve times, storing each new q in the array q(i). The graphic output shown in g-

Br H1 H0 '

ure 2 results. As you can see, q is approaching 0.6. If you would like to see the values generated by the program, appropriate print statements can be added.

0 10,000 20,000 30,000 40,000 Field intensity (ampere turns per meter) (a) Flux density (webers per square meter) 150

General comments Journal bearing type Rubbing bearings Oilimpregnated porous metal bearings Rollingelement bearings Hydrodynamic Hydrostatic Self-acting Externally fluid film fluid film gas bearings pressurized bearings bearings gas bearings

1000 2000 3000 Field intensity (ampere-turns per meter) (b)

Figure 2 Graphical output of the computer program from gure 1, with axis labels drawn in. The frequency of the a allele, q, begins at 0.1 and asymptotes toward 0.6.

200 400 600 Field intensity (ampere-turns per meter) (c)

(20.25)

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