Elements of Mechanical Design potx

44 156 0
Elements of Mechanical Design potx

Đang tải... (xem toàn văn)

Tài liệu hạn chế xem trước, để xem đầy đủ mời bạn chọn Tải xuống

Thông tin tài liệu

MIT OpenCourseWare http://ocw.mit.edu 2.72 Elements of Mechanical Design Spring 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms . 2.72 Elements of Mechanical Design Lecture 05: Structures Schedule and reading assignment © Martin Culpepper, All rights reserved Quizzes  Quiz – None Topics  Finish fatigue  Finish HTMs in structures Reading assignment  None  Quiz next time on HTMs 2 Matrix Review What is a Matrix? b A matrix is an easy way to 1 ⎤ ⎥ ⎦ ⎤ ⎥ ⎦ ⎡ represent a system of linear ⎢ b equations ⎣ 2 Linear algebra is the set of “Vector” rules that governs matrix ⎡ ⎢ ⎣ and vector operations a 1 a 2 a 3 a 4 “Matrix” © Martin Culpepper, All rights reserved 4 Matrix Addition/Subtraction You can only add or subtract matrices of the same dimension Operations are carried out entry by entry b b b b ⎤ + a a a a 1 2 1 2 1 1 2 2 ⎥ + ⎦ (2 x 2) (2 x 2) (2 x 2) − ⎤ ⎥ − ⎦ + = + b b b b + a a a a 3 4 3 4 3 3 4 4 − − ⎡ ⎢ ⎣ ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ b b b b ⎤ a a a a 1 2 1 2 1 1 2 2 ⎥ b b b ba a a a ⎦ 3 4 3 4 3 3 4 4 (2 x 2) (2 x 2) (2 x 2) − = ⎡ ⎢ ⎣ ⎡ ⎢ ⎣ © Martin Culpepper, All rights reserved ⎤ ⎥ ⎦ ⎤ ⎥ ⎦ ⎡ ⎢ ⎣ ⎡ ⎢ ⎣ 5 Matrix Multiplication ⎤ ⎥ ⎦ An matrix times an matrix produces an matrixm x n n x p m x p b b b b b b ++ a a a a a a 1 2 1 2 1 1 2 3 1 2 2 4 b b b b b b ++ a a a a a a 3 4 3 4 3 1 4 3 3 2 4 4 (2 x 2) (2 x 2) (2 x 2) = ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ © Martin Culpepper, All rights reserved ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ ⎡ ⎢ ⎣ 6 Matrix Properties © Martin Culpepper, All rights reserved Notation: A, B, C = matrix , c = scalar Cumulative Law: A + B = B + A Distributive Law: c(A + B) = cA + cB C(A + B) = CA + CB Associative Law: A + (B – C) = (A + B) – C A(BC) = (AB)C NOTE that AB does not equal BA !!!!!!! 7 Matrix Division © Martin Culpepper, All rights reserved To divide in linear algebra we multiply each side by an inverse matrix: AB = C A -1 AB = A -1 C B = A -1 C Inverse matrix properties: A -1 A = AA -1 = I (The identity matrix) (AB) -1 = B -1 A -1 8 Structures [...]... Cross-Sectional Area of large sections = Cross-Sectional Area of Drill Bit = Young’s Modulus of Material = © Martin Culpepper, All rights reserved 1 e E Ad A 0 0 0 1 -(D-δ) 0 0 1 δ= FD EAd 31 Drill Press Example Simple Beam Example: Find the HTM from b to c: L c b H a D c b F F cosӨ L e Cross-Sectional Area of large sections = Cross-Sectional Area of Drill Bit = Young’s Modulus of Material = © Martin... Cross-Sectional Area of large sections = Cross-Sectional Area of Drill Bit = Young’s Modulus of Material = © Martin Culpepper, All rights reserved E Ad c Hb = sinӨ cosӨ δ 0 d -sinӨ L 0 1 A FL3 δ= 3EI FL2 Ө= 2EI 34 Drill Press Example Simple Beam Example: Find the HTM from c to d: L c c b H a F FL D F d L e d cosӨ Cross-Sectional Area of large sections = Cross-Sectional Area of Drill Bit = Young’s Modulus of Material... 3 1 2 © Martin Culpepper, All rights reserved 12 Modeling: stick figures 1 Stick figures These types of models are idealizations of the physical behavior The designer must KNOW: 2 Beam bending 3 System bend (a) if beam bending assumptions are valid (b) how to interpret and use the results o this type of these models 3 1 2 © Martin Culpepper, All rights reserved y z x 13 Modeling: stick figures F © Martin... with structural design Machine concepts ‰ ‰ Topology Material properties Image removed due to copyright restrictions Please see http://www.fortune-cnc.com/uploads/images/1600ge_series.jpg Principles ‰ ‰ ‰ ‰ Thermomechanical Elastomechanics Kinematics Vibration Key tools that help ‰ ‰ Stick figures Parametric system/part error model © Martin Culpepper, All rights reserved Visualization of the: Load path... -sinӨ L 0 cosӨ D 0 0 1 1 FL3 D= 3EI FL2 Ө= 2EI 28 Drill Press Example Simple Beam Example: Find the HTM from a to b: L b c b H a D a F F d L Ha = b Cross-Sectional Area of large sections = Cross-Sectional Area of Drill Bit = Young’s Modulus of Material = © Martin Culpepper, All rights reserved 1 e A 0 0 0 1 -(D-δ) 0 0 1 Ad E 29 Useful Force-deflection Equations Force Deflection Equations d d= F d Ө FL EA...Machines structures Structure = backbone = affects everything Satisfies a multiplicity of needs ‰ ‰ ‰ Enforcing geometric relationships (position/orientation) Material flow and access Reference frame Requires first consideration and serves to link modules: ‰ ‰ ‰ ‰ ‰ ‰ ‰ Joints (bolted/welded/etc…) . http://ocw.mit.edu 2.72 Elements of Mechanical Design Spring 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms . 2.72 Elements of Mechanical Design Lecture. types of models are idealizations of the physical behavior. The designer must KNOW: (a) if beam bending assumptions are valid (b) how to interpret and use the results o this type of these. Principles  Thermomechanical  Elastomechanics  Kinematics  Vibration Key tools that help  Stick figures  Parametric system/part error model Visualization of the: Load path Vibration

Ngày đăng: 13/07/2014, 01:21

Tài liệu cùng người dùng

Tài liệu liên quan