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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 /3819/CH1/EX1.3 | |
parent | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (diff) | |
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initial commit / add all books
Diffstat (limited to '3819/CH1/EX1.3')
-rw-r--r-- | 3819/CH1/EX1.3/Ex1_3.sce | 12 |
1 files changed, 12 insertions, 0 deletions
diff --git a/3819/CH1/EX1.3/Ex1_3.sce b/3819/CH1/EX1.3/Ex1_3.sce new file mode 100644 index 000000000..d7be0dab3 --- /dev/null +++ b/3819/CH1/EX1.3/Ex1_3.sce @@ -0,0 +1,12 @@ +// A Textbook of Fluid Mecahnics and Hydraulic Machines - By R K Bansal
+// Chapter 1-Properties of Fluid
+// Problem 1.3
+
+y=poly(0,"y")
+u=2/3*y-y^2 // Defining the Velocity Function
+a=derivat(u) //Taking Derivative of the Velocity
+visc=8.63/10 //Converting Dynamic Viscosity from poise to N s/m^2
+ss1=visc*horner(a,0) //Shear stress=(Dynamic viscosity *Velocity Gradient) at y=0
+mprintf("The shear stress at y=0 is %f N/m^2 \n",ss1)
+ss2=visc*horner(a,0.15) //Shear stress=(Dynamic viscosity *Velocity Gradient) at y=0.15
+mprintf("The shear stress at y=0.15 is %f ",ss2)
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