Validation of Kirchoff's Plate Theory & its Applicability for Beams
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May 08, 2017
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Language: en
Added: May 08, 2017
Slides: 21 pages
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Validation of Kirchoff’s Plate Theory & its Applicability for Beams b y Abhishek Mondal (12NA30002) Department of Ocean Engineering & Naval Architecture IIT Kharagpur Under the guidance of : Prof. R. Datta Prof. N.Datta
Contents Kirchoff’s Plate Theory Problem Formulation Results : Thickness Variation Euler-Bernoulli’s Beam Theory Beam vs Plate Results : Aspect Ration Limitation Future Work References
Kirchoff’s Plate Theory It’s an extension of Euler-Bernoulli’s Beam theory to thin plates where aspect ratio is considerable Mid surface plane of a 3-D plate is used to construct a 2-D mathematical model to determine stresses & deformations Shear deformation and rotary inertia are ignored
Kirchoff’s Plate Theory The governing differential equation for an isotropic homogeneous plate is : Where h : Plate thickness E : Young’s Modulus q : Load per unit area ρ : Density ν : Poisson’s Ratio
Modelling Plate Area : 1 m x 1 m square section E = 210 GPa ρ = 7850 kg /m3 ν = 0.3 Boundary Conditions : i) Fixed Edge : z = 0 & z’ = 0 ii) Free Edge : z’’ = 0 & z’’’ = 0 iii) Sliding Edge : z’ = 0 & z’’’ = 0 iv) Hinged Edge : z = 0 & z’’ = 0
Beam Beams are nothing but a special case of plates where aspect ratio (L/B) to is high. It is subjected to transverse load only Moment acts about only one axis Load doesn’t vary in transverse direction
Euler–Bernoulli’s Beam Theory Euler-Bernoulli’s beam theory covers the case when deflection is very small compared to the length of the beam. The Euler-Bernoulli equation that describes the relationship between deflection and the applied load is :
Euler–Bernoulli’s Beam Theory When there is no external force acting on the beam q = 0 Solving the equation using separation of variable technique w = A 1 cos( β x)+A 2 sin( β x)+A 3 cosh( β x)+A 4 sinh( β x) w here
Euler–Bernoulli’s Beam Theory 4 types of beams has been considered viz., Simply Supported Beam [sin( β L )* sinh ( β L ) = 0] Cantilever Beam [ cos ( β L)* cosh ( β L) +1 = 0] Clamped Beam [ cos ( β L)* cosh ( β L) =1 ] Free Beam [ cos ( β L)* cosh ( β L) =1]
Simply Supported Beam β 1 L = 3.1416 β 2 L = 6.2832 β 3 L = 9.4248
Cantilever Beam β 1 L = 1.875 β 2 L = 4.694 β 3 L = 7.855
Clamped Beam β 1 L = 4.73 β 2 L = 7.853 β 3 L = 10.996
References Proof of convergence for a set of admissible functions for the Rayleigh–Ritz analysis of beams and plates and shells of rectangular platform - L.E . Monterrubio & S . Ilanko The Da Vinci-Euler-Bernoulli Beam Theory – Ballarini & Roberto http://iitg.vlab.co.in /?sub=62&brch=175&sim=1080&cnt=1