00:01
So here we are given that the viscosity of liquid can be determined with the rotation slender visco viscometer which is shown here in such a device.
00:12
So this device is shown here.
00:14
Here liquid is present in all this direction.
00:20
Here we are given the value of the r.
00:21
This is ri, this is ro, inner radius and outer radius.
00:26
Here we are given this shaft which is moving at the t with the angular velocity omega.
00:33
This is a fixed outer cylindrical and this is the liquid which is filled here.
00:40
So this value is given.
00:42
We have to apply the vector, stroke and continuity equation for this viscometer.
00:48
So here we have to apply the equation.
00:51
So here firstly we are about the assumption that there must be the 3d flow.
00:59
Next is that there can be incompressible flow.
01:06
Flow will be incompressible.
01:08
Next is that no flow or variation of properties in two directions.
01:16
So we are considering the value of v2 is 0 and sigma divided by sigma z that too is equal to 0.
01:22
Next from here is symmetry in the circumcenter that is sigma divided by sigma theta that too is equal to 0.
01:30
So we are considering about the navier -stokes and the continuity equation.
01:38
So from here we are considering about the continuity.
01:44
So equation will be 1 divided by r, sigma divided by the sigma r, r multiplied by the vn plus 1 by r, sigma divided by sigma theta multiplied by the v theta plus sigma divided by sigma z, vz that is equal to 0.
01:58
This term from here is u and this term from here is 3.
02:03
So the value of sigma divided by the sigma r multiplied by the r of vn is equal to 0.
02:08
So the value of r of vn from here is constant...