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                                Strength of Materials - Relationship 
                                  among the elastic constants |   
                            | 8.1. 
                                Relationship between modulus of elasticity and 
                                modulus of rigidity
 Consider a square element ABCD of side ‘a’ 
                                subjected to simple shear of intensity q as shown 
                                in figure.
 It is deformed to the shape AB’C’D 
                                under the shear stress. Drop perpendicular BE 
                                to the diagonal DB’. Let ? be the shear 
                                strain induced and let N be the modulus of rigidity.
 The diagonal DB gets elongated to DB’. Hence 
                                there is tensile strain et in the diagonal.
 et = (DB’ – DB) / DB = EB’ / 
                                DB
 since this deformation is very small we can take 
                                L BB’E = 45º
 EB’ = BB’ / v2 = AB tan ? / v2 = a 
                                tan ? / v2
 DB = v2 a
 et = (a tan ? / v2)/ v2 a = tan ? /2 = = ? / 2 
                                since ? is small
 ie et = ½ X q/N ------------------ (1)
 We know that stress along the diagonal DB is a 
                                pure tensile stress pt = q and that along the 
                                diagonal AC is a pure compressive stress pc also 
                                equal to q. hence the strain along the diagonal 
                                DB is et = q/E + 1/m X q/E
 Ie et = q/E (1+1/m) ------------------ (2)
 From (1) and (2) we have,
 E = 2N(1+1/m)
 This is the required relationship between E and 
                                N.
 
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                            | 8.2. 
                                Relationship between Modulus of Elasticity E and 
                                Bulk Modulus K
 
   
 Consider a cube element subjected to volumetric 
                                tensile stress p? in X,Y and Z directions. Stress 
                                in each direction is equal to p?. ie px = py = 
                                pz =p?
 Consider strains induced in X-direction by these 
                                stresses. px induces tensile strain , while py 
                                and pz induces compressive strains. Therefore,
 ex = px/E – 1/m[py/E + pz/E] = p?/E[1-2/m]
 due to the perfect symmetry in geometry and stresses
 ey = p?/E[1-2/m]
 ez = p?/E[1-2/m]
 K = p ? / e ? =p ?/(ex+ey+ez) = p?/[3p?/E(1-2/m)]
 ie E = 3K(1-2/m ) is the required relationship.
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                            |  8.3. 
                                Relationship among the constants
 From above,
 E = 2N[1+(1/m)] and E = 3K[1-(2/m )]
 E = 3K[1-2(E/2N -1)] = 3K[1-E/N +2]
 9K = E[1+(3K/N)] = E[(N+3K)/N]
 E = 9NK/(N+3K)
 
 9. Bars of uniform 
                                section
 
 Consider a bar of length l and Cross sectional 
                                area A. Let P be the axial pull on the bar,p the 
                                stresss induced ,e the strain in the bar and dl 
                                is the elongation.
 Then p= P/A
 e= p/E =P/(AE) -------------(1)
 e= dl/l -------------(2)
 equating (1) and (2)
 dl = Pl / (AE)
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