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of oblique solids, by introducing the idea of polarity in the axes of 

 crystallization, Mr. Dana has successfully applied this molecular 

 theory to crystallography, yet he goes no farther ; and the most im- 

 portant and difficult steps in this branch of physical science still re- 

 main to be made, and many phenomena in crystallization, with the 

 cause of which we are at present wholly unacquainted, still require 

 to be explained by the theory. The author particularly refers to 

 the important facts discovered by MM. Leblanc and Beudant, of 

 the influence that solutions or mediums in which bodies crystallize 

 have on the secondary forms which these bodies take ; and states, 

 that the present views of crystallography afford not even a glimpse 

 of the least relation between such forms and the properties of the 

 mediums. Why, he asks, does pure water appear, in general, to 

 tend to simplify the forms, precisely as do certain mixtures, those of 

 chlorite in axinite, quartz, felspar, &c., and why, on the contrary, 

 do other mediums, acid or earthy, complicate them ? 



Impressed with the importance which must attach to the solution 

 of such questions, M. Necker offers some ideas which long medita- 

 tion on this important subject has suggested to him. 



Adopting the ellipsoid as the form of the molecule, he remarks, 

 that the more complicated the form of the crystal, the more the 

 number of its faces increases, and the more, at the same time, does 

 it approach to the ellipsoidal form of the molecule ; and, on the con- 

 trary, the simpler the form becomes, the more does it recede from 

 that with a curved surface. All crystalline forms may be considered 

 as making a part of one or more series, which, in each system of 

 crystallization, have for extreme terms, on the one side, the most sim- 

 ple solid of the system, or that which has the least number possible 

 of faces, and on the other, the solid having the greatest number, 

 namely a sphere or an ellipsoid. Although it is more convenient in 

 the calculation of forms to start from the most simple polyhedral 

 forms in order to arrive at the more complex, nothing proves that 

 such has been the route which nature has followed. As long as we 

 considered the integral molecules as polyhedral, it appeared natural 

 to view them as grouping in polyhedrons ; but when once we cease 

 to admit polyhedral molecules, it then becomes most natural to sup- 

 pose, that ellipsoidal molecules should have a tendency, more or less 

 decided, to group in solids of the same form as themselves, when no 

 extraneous circumstances interpose an obstacle to this tendency. 



In order to give an idea of the kind of effect which would be pro- 

 duced on the form of the solid by these obstacles, such as the nature 

 of the medium in which crystallization takes place, a hurried or tu- 

 multuous crystallization, &c., the author conceives that each mole- 

 cule, as well as each solid formed by their union, has different axes 

 of attraction, endued with different degrees of energy, and symme- 

 trically disposed in groups, the weaker and the most numerous round 

 the stronger, which are, at the same time, the smallest in number ; 

 all, in short, symmetrically arranged around the principal axes of 

 crystallization, which are the most energetic of all. Thus we shall 

 conceive that sort of polarity by which crystallization is distin- 



