The Elastical Researches of Barré de Saint-Venant |
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Page viii
... molecular problems , its value as a key to the inmost recesses of Nature's laboratory , -is well brought out in much of Saint - Venant's work ; while on the other hand we find questions of impact , of plasticity , of combined strain and ...
... molecular problems , its value as a key to the inmost recesses of Nature's laboratory , -is well brought out in much of Saint - Venant's work ; while on the other hand we find questions of impact , of plasticity , of combined strain and ...
Page 3
... molécules . He thus starts from the molecular standpoint , but this definition does not appear to be absolutely necessary to the course of his reasoning . ( B ) On pp . 237-248 we have the analysis of strain . Here the slides first ...
... molécules . He thus starts from the molecular standpoint , but this definition does not appear to be absolutely necessary to the course of his reasoning . ( B ) On pp . 237-248 we have the analysis of strain . Here the slides first ...
Page 4
... molecular standpoint as follows : Nous appellerons donc en général Pression , sur un des deux côtes d'une petite ... molécules situées de ce côte sur les molécules du côté opposé , et dont les directions traversent cette face ; toutes ...
... molecular standpoint as follows : Nous appellerons donc en général Pression , sur un des deux côtes d'une petite ... molécules situées de ce côte sur les molécules du côté opposé , et dont les directions traversent cette face ; toutes ...
Page 54
... molecules m ' , m " to have length r , and projections x , y , z on the coordinate axes before strain . After strain x and z remain unchanged , but y will be increased by ys , owing to the stretch and xσ owing to 1 See the footnote to ...
... molecules m ' , m " to have length r , and projections x , y , z on the coordinate axes before strain . After strain x and z remain unchanged , but y will be increased by ys , owing to the stretch and xσ owing to 1 See the footnote to ...
Page 55
... molecules will be increased by the quantity A mutual action = ƒ ( r ) . ( ys , + Xσxy ) y will thus be developed between the molecules by the displacement , where f ( r ) is some function of r . If these molecules m ' , m " form part of ...
... molecules will be increased by the quantity A mutual action = ƒ ( r ) . ( ys , + Xσxy ) y will thus be developed between the molecules by the displacement , where f ( r ) is some function of r . If these molecules m ' , m " form part of ...
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Ave Maria Ave Maria Lane axes axis beam Boussinesq C. J. CLAY Cambridge University Press Christ's College CLAY & SONS Clebsch coefficients College Comptes rendus constant contour corps cosh cross-section Crown 8vo cylindrical d'une deduced deflection Demy 8vo deux distance dx² edition elasticity élastiques ellipsoidal equations fail-point flexure footnote formulae function given gives Hooke's Law hypothesis isotropy Lamé Leçons de Navier linear elasticity LL.D load longitudinal M₁ manière Maurice Lévy maximum memoir on Torsion molecules Notes obtained plane plastic plate prism problem rari-constant rectangular referred résistance rupture Saint-Venant Saint-Venant's shear shews shifts sinh slide solution St John's College strain stresses stretch stretch-modulus suppose surface terminal theory traction Trinity College U₁ University of Cambridge University Press Warehouse V₁ V₂ velocity Venant vibrations
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