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Diffstat (limited to '3862/CH11/EX11.10/Ex11_10.sce')
-rw-r--r-- | 3862/CH11/EX11.10/Ex11_10.sce | 80 |
1 files changed, 80 insertions, 0 deletions
diff --git a/3862/CH11/EX11.10/Ex11_10.sce b/3862/CH11/EX11.10/Ex11_10.sce new file mode 100644 index 000000000..e7b003d81 --- /dev/null +++ b/3862/CH11/EX11.10/Ex11_10.sce @@ -0,0 +1,80 @@ +clear +// + +P1=(20) //vertical loading from A at distance of 1m,KN. +P2=(20) //vertical loading from A at distance of 2m,KN. +P3=(20) //vertical loading from A at distance of 3m,KN. +Ra=(P1+P2+P3)/2 //Due to symmetry + +Rb=Ra +//At section 1.5 m from A +F=(Ra-P1)*1000 +M=((Ra*1.5-P1*0.5)*1000000) +b=(100) +h=(180) + +I=((b*(h**3))/12) + +// Bending stress +//f=M*y/I +y11=0 +f1=(-1)*M*y11/I +y22=45 +f2=(-1)*M*y22/I +y33=90 +f3=(-1)*M*y33/I +//Shearing stress at a fibre ‘y’ above N–A is +//q=(F/(b*I))*(A*y1) +//at y=0, +y1=45 +A1=b*90 +q1=(F/(b*I))*(A1*y1) +//at y=45 +y2=(90-45/2) +A2=b*45 +q2=(F/(b*I))*(A2*y2) +//at y=90 +q3=0 + +//(a) At neutral axis (y = 0) : The element is under pure shear + +py=0 + +p1=(f1+py)/2+sqrt((((f1-py)/2)**2)+(q1**2)) + +p2=(f1+py)/2-sqrt((((f1-py)/2)**2)+(q1**2)) +printf("\n (i) p1= %0.4f N/mm^2",p1) +printf("\n p2= %0.4f N/mm^2",p2) + +theta1=45 +theta2=theta1+90 +printf("\n theta= %0.0f ° and %0.0f °",theta1,theta2) + +//(b) At (y = 45) +py=0 + +p1=(f2+py)/2+sqrt((((f2-py)/2)**2)+(q2**2)) + +p2=(f2+py)/2-sqrt((((f2-py)/2)**2)+(q2**2)) +printf("\n (ii) p1= %0.4f N/mm^2",p1) +printf("\n p2= %0.4f N/mm^2",p2) + +thetab1=(atan((2*q2)/(f2-py))*180)/(%pi*2) +thetab2=thetab1+90 +printf("\n theta= %0.0f ° and %0.0f °",thetab1,thetab2) +//mistake in book +printf("\n mistake in book") + +//(c) At Y=90 + +py=0 + +p1=(f3+py)/2+sqrt((((f3-py)/2)**2)+(q3**2)) + +p2=(f3+py)/2-sqrt((((f3-py)/2)**2)+(q3**2)) +printf("\n (iii) p1= %e N/mm^2",p1) +printf("\n p2= %0.4f N/mm^2",p2) + +thetac1=(atan((2*q3)/(f3-py))*180)/(%pi*2) +thetac2=thetac1+90 +printf("\n theta= %0.0f ° and %0.0f °",thetac1,thetac2) |