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where the parameter is a scalar constant for a particular physical medium (at least, for the applications we consider here) and is called the permeability of the medium The permeability of a material can be factored as the product of the

A wild-type male is X-rayed and mated to a vermilion, miniature, sable female. Among the progeny is a single vermilion-eyed, long-winged, tan-bodied female. The following shows the progeny when this female is mated with a v m s hemizygous male.

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01 Simple orifices with circular pockets e = 05 For e = 09 multiply C L by 165 0 0 05 10 15 20 25 30

Table 161 Relative permeabilities for common materials Material Air Permalloy Cast steel Sheet steel Iron r 1 100,000 1,000 4,000 5,195

Females 87 vermilion, miniature, sable 93 vermilion Males 89 vermilion, miniature, sable 1 vermilion

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permeability of free space, 0 = 4 10 7 H/m, times the relative permeability, r , which varies greatly according to the medium For example, for air and for most electrical conductors and insulators, r is equal to 1 For ferromagnetic materials, the value of r can take values in the hundreds or thousands The size of r represents a measure of the magnetic properties of the material A consequence of Amp` re s law is that, the larger the value of , the smaller the current required to e produce a large ux density in an electromagnetic structure Consequently, many electromechanical devices make use of ferromagnetic materials, called iron cores, to enhance their magnetic properties Table 161 gives approximate values of r for some common materials Conversely, the reason for introducing the magnetic eld intensity is that it is independent of the properties of the materials employed in the construction of magnetic circuits Thus, a given magnetic eld intensity, H, will give rise to different ux densities in different materials It will therefore be useful to de ne sources of magnetic energy in terms of the magnetic eld intensity, so that different magnetic structures and materials can then be evaluated or compared for a given source In analogy with electromotive force, this source will be termed magnetomotive force (mmf) As stated earlier, both the magnetic ux density and eld intensity are vector quantities; however, for ease of analysis, scalar elds will be chosen by appropriately selecting the orientation of the elds, wherever possible Amp` re s law states that the integral of the vector magnetic eld intensity, e H, around a closed path is equal to the total current linked by the closed path, i: H dl = i (1620)

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where dl is an increment in the direction of the closed path If the path is in the same direction as the direction of the magnetic eld, we can use scalar quantities to state that H dl = i (1621)

Explain these results by drawing a genetic map. 15. In Drosophila, recessive genes clot (ct) and black body (b) are located at 16.5 and 48.5 map units, respectively, on the second chromosome. In one cross, wild-type females that are ct b /ct b are mated with ct b/ct b males. They produce these progeny:

Figure 169 illustrates the case of a wire carrying a current i, and of a circular path of radius r surrounding the wire In this simple case, you can see that the magnetic eld intensity, H, is determined by the familiar right-hand rule This rule states that if the direction of the current i points in the direction of the thumb of one s right hand, the resulting magnetic eld encircles the conductor in the direction in which the other four ngers would encircle it Thus, in the case of Figure 169, the closed-path integral becomes equal to H (2 r), since the path and the magnetic eld are in the same direction, and therefore the magnitude of the magnetic eld intensity is given by H = i 2 r (1622)

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