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author | priyanka | 2015-06-24 15:03:17 +0530 |
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committer | priyanka | 2015-06-24 15:03:17 +0530 |
commit | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (patch) | |
tree | ab291cffc65280e58ac82470ba63fbcca7805165 /3289/CH4 | |
download | Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.tar.gz Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.tar.bz2 Scilab-TBC-Uploads-b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b.zip |
initial commit / add all books
Diffstat (limited to '3289/CH4')
-rwxr-xr-x | 3289/CH4/EX4.1/Ex4_1.sce | 47 | ||||
-rwxr-xr-x | 3289/CH4/EX4.3/EX4_3.sce | 43 | ||||
-rwxr-xr-x | 3289/CH4/EX4.4/Ex4_4.sce | 22 | ||||
-rwxr-xr-x | 3289/CH4/EX4.5/Ex4_5.sce | 27 | ||||
-rwxr-xr-x | 3289/CH4/EX4.6/Ex4_6.sce | 50 | ||||
-rwxr-xr-x | 3289/CH4/EX4.7/Ex4_7.sce | 43 |
6 files changed, 232 insertions, 0 deletions
diff --git a/3289/CH4/EX4.1/Ex4_1.sce b/3289/CH4/EX4.1/Ex4_1.sce new file mode 100755 index 000000000..40f90ee61 --- /dev/null +++ b/3289/CH4/EX4.1/Ex4_1.sce @@ -0,0 +1,47 @@ +clc;
+
+sigmayp=350 //MPa
+sigma3=0
+M=8 //kN
+Mt=24 //kNm
+N=2
+v=0.3
+
+// sigma= My/I ==32M/%pid^3
+// tau= Mt*r/J ==16Mt/%pid^3
+//sigma1=(16*(M+sqrt(M^2+Mt^2)))/(%pi*d^3)
+//sigma2=(16*(M-sqrt(M^2+Mt^2)))/(%pi*d^3)
+
+//solution a: max principal stress theory
+//(16*(M+sqrt(M^2+Mt^2)))/(%pi*d^3)=sigmayp/N
+
+a=(16*(M+sqrt(M^2+Mt^2)))/%pi
+disp(a)
+b=sigmayp*10^6/N
+disp(b)
+d=(a/b)^(1/3)
+disp(d,"diameter of the bar in meter is= ")
+
+//solution b:max shearing stress theory
+
+c=(32*sqrt(M^2+Mt^2))/%pi
+disp(c)
+d=(c/b)^(1/3)
+disp(d,"diameter of the bar in meter is= ")
+
+//solution c:max principal strain theory
+//epsilon1=(sigma1-v(sigma2+sigma3))/E=epsilonyp/N=sigmayp/EN Or
+//sigma1-v(sigma2+sigma3)=b given
+//sigma1=b+v(sigma2+sigma3) substituting the values of the sigma 1,2 and 3 we get
+//(16*(M+sqrt(M^2+Mt^2)-vM-v*sqrt(M^2+Mt^2)))/(%pi*d^3)=b
+e=(16*(M+sqrt(M^2+Mt^2)-v*M-v*sqrt(M^2+Mt^2)))/%pi
+disp(e)
+d=(e/b)^(1/3)
+disp(d,"diameter of the bar in meter is= ")
+
+//solution d:max energy of distortion theory
+
+f=(16*sqrt(4*M^2+3*Mt^2))/%pi
+disp(f)
+d=(f/b)^(1/3)
+disp(d,"diameter of the bar in meter is= ")
diff --git a/3289/CH4/EX4.3/EX4_3.sce b/3289/CH4/EX4.3/EX4_3.sce new file mode 100755 index 000000000..de12c5daf --- /dev/null +++ b/3289/CH4/EX4.3/EX4_3.sce @@ -0,0 +1,43 @@ +clc
+
+sigmau1=300 //MPa
+sigmau2=700 //MPa
+b=0.105 //m outer diameter
+a=0.100 //m inner diameter
+
+//sigma1==(-sigma2)==tau
+
+sigma3=0
+
+//Mt=J*tau/r= (%pi*(b^2-a^2))/2*b
+//Mt=((%pi*(b^4-a^4))/(2*b))*tau equation a
+q=(%pi*(b^4-a^4))/(2*b)
+
+//solution a: max principal stress theory
+tau=sigmau1
+Mt=q*tau*10^6
+disp(Mt,"max principal stress in Nm is= ")
+
+//solution b:max shearing stress theory
+// |sigma1-sigma2|=sigmau1
+// 2*sigma1==sigmau1==2*tau or
+
+Mt=q*tau*10^6
+disp(Mt,"max shearing stress in Nm is= ")
+
+//solution c:Coulomb- mohr theory
+//(tau/sigmau1)-(-tau/sigmau2)=1
+tau=1*((sigmau1*sigmau2)/(sigmau1+sigmau2))
+disp(tau,"tau in MPa is= ")
+Mt=q*tau*10^6
+disp(Mt,"Coulomb- mohr in Nm is= ")
+
+
+
+
+
+
+
+
+
+
diff --git a/3289/CH4/EX4.4/Ex4_4.sce b/3289/CH4/EX4.4/Ex4_4.sce new file mode 100755 index 000000000..0df8e6719 --- /dev/null +++ b/3289/CH4/EX4.4/Ex4_4.sce @@ -0,0 +1,22 @@ +clc
+
+a=0.05 // m
+Fm=90 //kN
+sigmacr=210 // MPa
+sigmayp=280 // MPa
+
+//sigmaa=Ma*c/I equation 1
+//Ma=0.025*Fa
+c=0.025
+I=(a^4)/12
+disp(I)
+//sigmaa=((0.025*Fa)*c)/I substituting the values
+
+
+//sigmam=Fm/A equation 2
+sigmam=Fm/(a*a)
+disp(sigmam,"in kilo Pa is= ")
+
+//(((1200*Fa)/sigmacr)+(sigmam/sigmayp))=1
+Fa=(1-(sigmam/sigmayp))*(sigmacr/1200)
+disp(Fa,"load Fa in N is= ") //wrong ans in textbook
diff --git a/3289/CH4/EX4.5/Ex4_5.sce b/3289/CH4/EX4.5/Ex4_5.sce new file mode 100755 index 000000000..f785f9700 --- /dev/null +++ b/3289/CH4/EX4.5/Ex4_5.sce @@ -0,0 +1,27 @@ +clc
+
+r=0.04 //m
+t=5 //mm
+sigmae=250 //MPa
+sigmay=300 //MPa
+
+//sigmathetamax=(p*r)/t =8*p max values of tangential stresses
+//sigmathetamin=((-p/4)*r)/t =-2*p min values of tangential stresses
+//sigmazamax=(p*r)/2*t =4*p axial principal stresses
+//sigmazmin=((-p/4)*r)/2*t =-p
+
+//sigmathetaa=(sigmathetamax-sigmathetamin)/2= 5p alternating and mean stresses
+//sigmathetam=(sigmathetamax+sigmathetamin)/2= 3p
+//sigmaza=(sigmazamax-sigmazmin)/2 =2.5p
+//sigmazm=(sigmazamax+sigmazmin)/2 =1.5p
+
+//sqrt(sigmathetaa^2-sigmathetaa*sigmaza+sigmaza^2)=sigmaea
+//sqrt(sigmathetam^2-sigmathetam*sigmazm+sigmazm^2)=sigmaem
+
+//sqrt(25p^2-12.3p^2+6.25p^2)=sigmaea
+//sqrt(9p^2-4.5p^2+2.25p^2)=sigmaem solving this equation we get
+sigmaea=4.33 //p
+sigmaem=2.60 //p
+
+p=1/((sigmaea/sigmae)+(sigmaem/sigmay))
+disp(p,"the value of p in MPa is= ")
diff --git a/3289/CH4/EX4.6/Ex4_6.sce b/3289/CH4/EX4.6/Ex4_6.sce new file mode 100755 index 000000000..bf4bdc443 --- /dev/null +++ b/3289/CH4/EX4.6/Ex4_6.sce @@ -0,0 +1,50 @@ +clc
+
+a=[700 14 0; 14 -350 0; 0 0 -350]
+disp(a)
+c=[-660 -7 0; -7 -350 0; 0 0 -350]
+disp(c)
+sigmau=2400 //MPa
+K=1
+sigmae=800 //MPa
+Nf=1 //cycles for SAE
+Nff=10^3 //cycles for Gerber
+Ne=10^8 //cycles
+
+sigmaxa=(700+660)/2
+disp(sigmaxa,"alternating and mean values of stresses in MPa is= ")
+sigmaxm=(700-660)/2
+disp(sigmaxm,"alternating and mean values of stresses in MPa is= ")
+sigmaya=(-350+350)/2
+disp(sigmaya,"alternating and mean values of stresses in MPa is= ")
+sigmaym=(-350-350)/2
+disp(sigmaym,"alternating and mean values of stresses in MPa is= ")
+sigmazm=(-350-350)/2
+disp(sigmazm,"alternating and mean values of stresses in MPa is= ")
+tauxya=(14+7)/2
+disp(tauxya,"alternating and mean values of stresses in MPa is= ")
+tauxym=(14-7)/2
+disp(tauxym,"alternating and mean values of stresses in MPa is= ")
+
+sigmaea=sqrt(((sigmaxa-sigmaya)^2+(sigmaya-sigmaxa)^2+6*(tauxya)^2)/2)
+disp(sigmaea,"in MPa is =")
+sigmaem=sqrt(((sigmaxm-sigmaym)^2+(sigmaym-sigmaxm)^2+6*(tauxym)^2)/2)
+disp(sigmaem,"in MPa is= ")
+
+//solution a:
+sigmacr=sigmaea/(1-(sigmaem/2400))
+disp(sigmacr)
+b=log(sigmau/sigmae)/log(1/Ne)
+disp(b)
+
+Ncr=1*(sigmacr/2400)^(1/b)
+disp(Ncr,"in cycles is= ")
+
+//solution b:
+sigmacr=sigmaea/(1-(sigmaem/sigmau)^2)
+disp(sigmacr,"in MPa is= ")
+b=log(0.9*2400/sigmae)/log(Nff/Ne)
+disp(b)
+
+Ncr=Nff*(sigmacr/(0.9*2400))^(-11.587)
+disp(Ncr,"in cycles is= ")
diff --git a/3289/CH4/EX4.7/Ex4_7.sce b/3289/CH4/EX4.7/Ex4_7.sce new file mode 100755 index 000000000..1be3ce0ba --- /dev/null +++ b/3289/CH4/EX4.7/Ex4_7.sce @@ -0,0 +1,43 @@ +clc
+
+W=180 //N
+h=0.1 //m
+L=1.16 //m
+w=0.025 //m
+d=0.075 //m
+E=200 //GPa
+k=180 //kN/m
+
+I=w*d^3
+disp(I)
+//deltast=(W*L^3)/(48*E*I) equation 1
+deltast=(W*L^3*12)/(48*E*10^9*I)
+disp(deltast,"deflection of a point in meter is= ")
+
+//deltastmax=Mc/I equation 2
+deltastmax=(W*L*12*0.0375)/(4*I)
+disp(deltastmax,"deflection of a point in Pa is= ")
+
+//solution a:
+a=1+sqrt(1+((2*h)/deltast))
+disp(a,"imapct factor is= ")
+deltamax=deltast*a
+disp(deltamax,"in meter is =")
+sigmamax=deltastmax*a
+disp(sigmamax,"in Pa is= ")
+
+//solution b:
+deltast=deltast+(90/180000)
+disp(deltast,"static deflection of the beam in meter is= ")
+a=1+sqrt(1+((2*h)/deltast))
+disp(a,"imapct factor is= ")
+deltamax=deltast*a
+disp(deltamax,"in meter is =")
+sigmamax=deltastmax*a
+disp(sigmamax,"in Pa is= ")
+
+
+
+
+
+
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