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Mechanics of Materials: Beam Deflections Engineered by Group 20  Christopher Webb, Anthony Williams, Carlaton Wong,  Jonathan Wong 03/03/2010
The Concept Scenario: How much will a beam deflect with an applied load? Calculating the beam’s deflection will reveal the beams curvature relationships This project is designed to exhibit the mechanics of a bending moment on a single cantilever beam. Ultimately leading us to our goal.
Goals & Objectives Experimental Goals How much will aluminum and brass deflect with various applied loads? Determine the Young’s Modulus based on the deflection measured Does our calculated Young’s Modulus equal tabulated values?
Beam Failures
What is Beam Deflection? When loads are applied to a beam, the beam’s axis that was once straight will become curved. The displacements from the initial axis are called bending or flexural deflections.
Apparatus Design & Operation ,[object Object]
At the end of the beam there will be an attachment to serve as the applied load.
This experiment used strategically filled water bottles for the applied loads.,[object Object]
Cantilever beams are interchangeable allowing for supplemental testing of differing materials & structural make-ups .
Negligible factors:
Load’s tiny distance from free end of member
Small bend in beam after multiple loads,[object Object]
Our Cantilever Beam
Superposition Table
MatLab Code hold on; grid on plot(x/in_m,v2*100,'g-*',x/in_m,v1*100,'ro-',x/in_m,v1*100+v2*100,'b*-') title('Beam Deflection of Brass w/ 0.3lb Load') xlabel('Beam Length (in)') ylabel('Deflection (cm)') legend('DistributedLoad','ConcentratedLoad','Total Deflection',3) V_max=(q*L+F)/(b*h);%Max shear stress sigma_max=(.5*q*L^2+F*L)*(h*0.5)/I; v_max_tot=(v1(end)+v2(end))*100;           %Analysis of Aluminum Beam close all;clearall;clc %Conversion Factors in_m=0.0254; %inch to meter  lb_N=0.22481;%Pound force to Newton  %Material Properties E=69*10^9;%Pa Aluminum %Geometric Properties(in SI units) %Al bar data h=(1/8)*in_m;%Cross section height b=(3/4)*in_m;%Cross sect width L=15*in_m;%Length of Beam (m) I=(b*h^3)/12; %second momemnt of inertia(m^4) %Analysis of Brass beam close all;clearall;clc %Conversion Factors in_m=0.0254; %inch to meter  lb_N=0.22481;%Pound force to Newton  %Material Properties E=100*10^9;%Pa Brass %Geometric Properties(in SI units) %Brass Bar data h=(.064)*in_m;%Cross section height b=(3/4)*in_m;%Cross sect width L=9*in_m;%Length of Beam (m) I=(b*h^3)/12; %second momemnt of inertia(m^4) %Applied force F=(.3)/lb_N; %(N) %Calculating deflection x=linspace(0,L,50); v1=(F*x.^3/6 - F*L*x.^2/2)/(E*I); %Deflection due to concentrated load q=79.7*10^-3*9.81/(12*.0254); v2=zeros(1,length(x)); for i=1:length(x) v2(i)=-q*x(i)^2/(24*E*I)*(6*L^2-4*L*x(i) + x(i)^2); %Deflection due to weight of bar end %Applied force F=(.3)/lb_N; %Calculating deflection     %Concetrated load x=linspace(0,L,50);     v1=(F*x.^3/6 - F*L*x.^2/2)/(E*I);%Deflection in (m)     %Distributed weight q=74*10^-3*9.81/(18.5*.0254);     v2=zeros(1,length(x));     for i=1:length(x)      v2(i)=-q*x(i)^2/(24*E*I)*(6*L^2-4*L*x(i) + x(i)^2);     end hold on;grid on;     plot(x/in_m,v1*100,'ro',x/in_m,v2*100,'g*',x/in_m,v1*100+v2*100,'b*') title('Beam Deflection of Aluminum w/ 0.3lb Load') xlabel('Beam Length (in)') ylabel('Deflection (cm)') legend('DistributedLoad','ConcentratedLoad','Total Deflection',3) V_max=(q*L+F)/(b*h)%Max shear stress sigma_max=(.5*q*L^2+F*L)*(h*0.5)/I; v_max_tot=(v1(end)+v2(end))*100;
Experiment Variables ,[object Object]
 Calculated Linear Weight Density by weighing the beams on a scale.
 Water bottles with a known mass used to calculate forces applied to the beam.,[object Object]
Results – Brass Bar .3 Lbs Force .4 Lbs Force .5 Lbs Force
Results – Aluminum Bar .3 Lbs Force .4 Lbs Force .5 Lbs Force
Experimental Results Aluminum : Expected Young’s Modulus: 69 GPa Brass: Expected Young’s Modulus: 100 GPa

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Mechanical of Materials

  • 1. Mechanics of Materials: Beam Deflections Engineered by Group 20 Christopher Webb, Anthony Williams, Carlaton Wong, Jonathan Wong 03/03/2010
  • 2. The Concept Scenario: How much will a beam deflect with an applied load? Calculating the beam’s deflection will reveal the beams curvature relationships This project is designed to exhibit the mechanics of a bending moment on a single cantilever beam. Ultimately leading us to our goal.
  • 3. Goals & Objectives Experimental Goals How much will aluminum and brass deflect with various applied loads? Determine the Young’s Modulus based on the deflection measured Does our calculated Young’s Modulus equal tabulated values?
  • 5. What is Beam Deflection? When loads are applied to a beam, the beam’s axis that was once straight will become curved. The displacements from the initial axis are called bending or flexural deflections.
  • 6.
  • 7. At the end of the beam there will be an attachment to serve as the applied load.
  • 8.
  • 9. Cantilever beams are interchangeable allowing for supplemental testing of differing materials & structural make-ups .
  • 11. Load’s tiny distance from free end of member
  • 12.
  • 15. MatLab Code hold on; grid on plot(x/in_m,v2*100,'g-*',x/in_m,v1*100,'ro-',x/in_m,v1*100+v2*100,'b*-') title('Beam Deflection of Brass w/ 0.3lb Load') xlabel('Beam Length (in)') ylabel('Deflection (cm)') legend('DistributedLoad','ConcentratedLoad','Total Deflection',3) V_max=(q*L+F)/(b*h);%Max shear stress sigma_max=(.5*q*L^2+F*L)*(h*0.5)/I; v_max_tot=(v1(end)+v2(end))*100;           %Analysis of Aluminum Beam close all;clearall;clc %Conversion Factors in_m=0.0254; %inch to meter lb_N=0.22481;%Pound force to Newton %Material Properties E=69*10^9;%Pa Aluminum %Geometric Properties(in SI units) %Al bar data h=(1/8)*in_m;%Cross section height b=(3/4)*in_m;%Cross sect width L=15*in_m;%Length of Beam (m) I=(b*h^3)/12; %second momemnt of inertia(m^4) %Analysis of Brass beam close all;clearall;clc %Conversion Factors in_m=0.0254; %inch to meter lb_N=0.22481;%Pound force to Newton %Material Properties E=100*10^9;%Pa Brass %Geometric Properties(in SI units) %Brass Bar data h=(.064)*in_m;%Cross section height b=(3/4)*in_m;%Cross sect width L=9*in_m;%Length of Beam (m) I=(b*h^3)/12; %second momemnt of inertia(m^4) %Applied force F=(.3)/lb_N; %(N) %Calculating deflection x=linspace(0,L,50); v1=(F*x.^3/6 - F*L*x.^2/2)/(E*I); %Deflection due to concentrated load q=79.7*10^-3*9.81/(12*.0254); v2=zeros(1,length(x)); for i=1:length(x) v2(i)=-q*x(i)^2/(24*E*I)*(6*L^2-4*L*x(i) + x(i)^2); %Deflection due to weight of bar end %Applied force F=(.3)/lb_N; %Calculating deflection %Concetrated load x=linspace(0,L,50); v1=(F*x.^3/6 - F*L*x.^2/2)/(E*I);%Deflection in (m) %Distributed weight q=74*10^-3*9.81/(18.5*.0254); v2=zeros(1,length(x)); for i=1:length(x) v2(i)=-q*x(i)^2/(24*E*I)*(6*L^2-4*L*x(i) + x(i)^2); end hold on;grid on; plot(x/in_m,v1*100,'ro',x/in_m,v2*100,'g*',x/in_m,v1*100+v2*100,'b*') title('Beam Deflection of Aluminum w/ 0.3lb Load') xlabel('Beam Length (in)') ylabel('Deflection (cm)') legend('DistributedLoad','ConcentratedLoad','Total Deflection',3) V_max=(q*L+F)/(b*h)%Max shear stress sigma_max=(.5*q*L^2+F*L)*(h*0.5)/I; v_max_tot=(v1(end)+v2(end))*100;
  • 16.
  • 17.
  • 18. Calculated Linear Weight Density by weighing the beams on a scale.
  • 19.
  • 20. Results – Brass Bar .3 Lbs Force .4 Lbs Force .5 Lbs Force
  • 21. Results – Aluminum Bar .3 Lbs Force .4 Lbs Force .5 Lbs Force
  • 22. Experimental Results Aluminum : Expected Young’s Modulus: 69 GPa Brass: Expected Young’s Modulus: 100 GPa
  • 23. Expected Results Aluminum: Brass: All measured deflections are higher than calculated. Why?
  • 24. Max Stress in Beam Using the Flexural formula and observing that the Mmax is located at the origin we can derive an expression for Pmax
  • 25.
  • 27.
  • 28. Mechanics of Materials:Beam Deflections Group 20 Christopher Webb, Anthony Williams, Carlaton Wong, & Jonathan Wong Thank you!