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HW6 Solutions

Course: 125 208, Spring 2011
School: Rutgers
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Introduction 14:125:208: to Biomechanics Homework Assignment #6 Spring 2007 Due 3/27/07 Problem 7: A paraplegic patient weighing 70kg is performing a pushup in the prone position (below). The lower legs and hands are supported by the floor. The force plate, placed under the right hand, shows a vertical force of 200N. The radius and ulna make a 75 degree angle with the horizontal. The triceps (thick black line),...

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Introduction 14:125:208: to Biomechanics Homework Assignment #6 Spring 2007 Due 3/27/07 Problem 7: A paraplegic patient weighing 70kg is performing a pushup in the prone position (below). The lower legs and hands are supported by the floor. The force plate, placed under the right hand, shows a vertical force of 200N. The radius and ulna make a 75 degree angle with the horizontal. The triceps (thick black line), which connects the olecranon process to the humerus, makes a 15 degree angle with the horizontal, and is assumed to connect at the proximal end of the lower arm. Assume that the geometry of the lower arm can be approximated as a hollow cylinder, with inner and outer radii, and resulting cross-sectional area and moment of inertia, as shown. You may assume that the geometry of the lower arm is uniform along its entire length. Conduct a biomechanical analysis of the lower arm, assuming that it acts as a beam. This should include: i) A free body diagram ii) A full beam analysis, including shear and bending moment diagrams iii) Calculation of the magnitude and location (relative to the length along the axis and position in a cross-section) of the maximum tensile the AND maximum compressive stresses. You can assume that all external loads act at the center of the cross-section of the bone. What about a beam in 3 point bending without symmetry? From statics we find the reaction forces R1 and R2 M ( x) = R1 x = M ( x) = Pb x L 0< x<a Pb x P(x a ) a < x < L L For these type of problems we have to evaluate the moment along the length of the beam First lets evaluate the deflection from x=0 to x=a M ( x) = R1 x = M ( x) = On the left support we find y(0)=0 so C2=0 Pb x L 0< x<a Pb x P(x a ) a < x < L L d 2 y Pb EI 2 = x dx L dy Pb x 2 = + C1 EI dx L2 Pb x 3 + C1 x + C2 EIy = L6 Pb x 3 + C1 x EIy = L6 11 Now lets evaluate from a<x<L d 2 y Pb x P(x a ) = dx 2 L 2 dy Pb x 2 P( x a ) EI = + C3 2 dx L2 3 Pb x 3 P( x a ) EIy = + C3 x + C 4 6 L6 Pb a 3 EIy (a ) = + C3 a + C 4 C 4 = 0 L6 C1 = C3 EI At point x=a Pb a 3 EIy(a ) = + C1a L6 Pb L3 P(L a ) + C3 L = 0 L6 6 3 P(b ) PbL2 Pb 2 C3 L = b L2 C1 = C3 = 6 6 6L Pb 3 EIy ( x ) = x L2 b 2 x 6L Pb 3 L 3 2 2 EIy ( x ) = x (x a ) L b x = 0 6L b 3 EIy(L ) = ( ( ( )) ( ) ) 0< x<a a<x<L 12
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