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author | prashantsinalkar | 2017-10-10 12:27:19 +0530 |
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committer | prashantsinalkar | 2017-10-10 12:27:19 +0530 |
commit | 7f60ea012dd2524dae921a2a35adbf7ef21f2bb6 (patch) | |
tree | dbb9e3ddb5fc829e7c5c7e6be99b2c4ba356132c /3594/CH15/EX15.11/Ex15_11.sce | |
parent | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (diff) | |
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initial commit / add all books
Diffstat (limited to '3594/CH15/EX15.11/Ex15_11.sce')
-rw-r--r-- | 3594/CH15/EX15.11/Ex15_11.sce | 28 |
1 files changed, 28 insertions, 0 deletions
diff --git a/3594/CH15/EX15.11/Ex15_11.sce b/3594/CH15/EX15.11/Ex15_11.sce new file mode 100644 index 000000000..9be8a056d --- /dev/null +++ b/3594/CH15/EX15.11/Ex15_11.sce @@ -0,0 +1,28 @@ +//to find the natural frequencies of the torsional vibration of the system when inertia is neglected and when it is taken into account
+clc
+//given
+g=32.3//ft/s^2
+l2=25.5//in
+d1=2.75//in
+d2=3.5//in
+C=12*10^6//modulus of rigidity
+G=1/0.6//given speed ratio
+Ib=54//lb in^2
+Ic=850//lb in^2
+Id=50000//lb in^2
+Id1=Id/G^2//15.62
+Ia=1500//lb in^2
+la=Id1/(Id1+Ia)*66.5
+J=%pi*d1^4/32
+q=C*J/la//torsional stiffness
+n=(1/(2*%pi))*(q*g*12/Ia)^(1/2)
+nf=n*60//for minutes
+//case b)
+Ib1=Ib+Ic/(G^2)
+a=63.15//in; distance of the node from rotor A (given)
+b=3.661//in; distance of the node from rotor A (given)
+N1=n*(la/a)^(1/2)
+N2=n*(la/b)^(1/2)
+N1f=N1*60//for minutes
+N2f=N2*60//for minutes
+printf("\na) The frequency of torsional vibrations n = %.1f per sec or %.f per min\nb) The fundamental frquency = %.1f per sec or %.f per min\n and the two node frequency = %.f per sec or %.f per min",n,nf,N1,N1f,N2,N2f)
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