mcoll
Mechanical
- Oct 22, 2002
- 10
Hi everyone,
Can anyone point me in the right direction for calculating a pressure requirement for my system.
I'm extruding a polymer (pneumatically) from a reservoir through a connection tube and out through a (circular) die, the discharge rate required is 25mm/s.
1.Being of such high viscosity I assume a laminar flow.
2.There is no heat transfer across the boundary of the system so that q = 0 and the heat energy generated by material shearing and friction at the wall is negligible.(This is not true, but I intend to deal with this aspect as and when I have grasped the dynamics of this basic system)
3.The change in height across the system is small so that z1 = z2
4.The material is considered uncompressible.
5.There is no work done by the fluid so that w=0.
I have therefore derived that:
K.½r.u² -- Inlet Losses
K.½r.u3² -- Outlet Losses
4FL/D .½r.u² -- Friction losses at wall (shear)
Where; ½r.u² = Dynamic Pressure (r - rho-density)
K = 0.5 (90 Degree)
Therefore:
4F1L1/D1 .½r.u1² + K1.½r.u1² + 4F2L2/D2 .½r.u2² + K2.½r.u2² + 4F3L3/D3 .½r.u3² + K3.½r.u3²
(can supply a diagram for anyone who is sufficiently interested).
The figures I get back are clearly wrong, even when I calulate for water (still laminar flow).
Can anyone reccommend another way (possibly other than an enengy equlibrium equasion) to calculater a force/pressure required at the piston (D1) to achieve the stated discharge rate?
Thanks in advance for any help, and well done for reading all of this post!
MC
Can anyone point me in the right direction for calculating a pressure requirement for my system.
I'm extruding a polymer (pneumatically) from a reservoir through a connection tube and out through a (circular) die, the discharge rate required is 25mm/s.
1.Being of such high viscosity I assume a laminar flow.
2.There is no heat transfer across the boundary of the system so that q = 0 and the heat energy generated by material shearing and friction at the wall is negligible.(This is not true, but I intend to deal with this aspect as and when I have grasped the dynamics of this basic system)
3.The change in height across the system is small so that z1 = z2
4.The material is considered uncompressible.
5.There is no work done by the fluid so that w=0.
I have therefore derived that:
K.½r.u² -- Inlet Losses
K.½r.u3² -- Outlet Losses
4FL/D .½r.u² -- Friction losses at wall (shear)
Where; ½r.u² = Dynamic Pressure (r - rho-density)
K = 0.5 (90 Degree)
Therefore:
4F1L1/D1 .½r.u1² + K1.½r.u1² + 4F2L2/D2 .½r.u2² + K2.½r.u2² + 4F3L3/D3 .½r.u3² + K3.½r.u3²
(can supply a diagram for anyone who is sufficiently interested).
The figures I get back are clearly wrong, even when I calulate for water (still laminar flow).
Can anyone reccommend another way (possibly other than an enengy equlibrium equasion) to calculater a force/pressure required at the piston (D1) to achieve the stated discharge rate?
Thanks in advance for any help, and well done for reading all of this post!
MC