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Section summary |
---|
1. Total pressure
drop on the tube side |
2. Pressure drop
inside the tubes |
3. Calculation of the pressure drop in inlet and return nozzles |
4. Calculation of the pressure drop in the return cover |
The pressure drop on the tube side of a shell-tubes heat exchanger is made of several components : the pressure drop in the inlet nozzle, the pressure drop in the outlet nozzle, the pressure drop in the return cover and the pressure drop through the tubes.
ΔPt = ΔPi + ΔPo + ΔPtubes+ ΔPc
With
ΔPt = total pressure drop in the heat exchanger (tube
side)
ΔPi = pressure drop in the inlet nozzle
ΔPo = pressure drop in the outlet nozzle
ΔPtubes = pressure drop in the tubes
ΔPc = pressure drop in the return cover
The Bell Delaware method expresses the pressure drop inside the shell with the following formula :
ΔPtubes = 2.f.ρ.V2.Lt.Φ/di
With
ΔPtubes = pressure drop in the tubes (Pa)
f = friction factor
ρ = density of the fluid (kg/m3)
V = fluid velocity in tubes (m/s)
Lt = total length of flow inside tubes (m)
di = inside diameter of the tubes (m)
Φ = correction factor for non isothermal flow
The following equation allows to calculate the pressure drop :
f = 0.0014+0.125*Re-0.32
(for Re>2100)
To be noted that the friction factor can be calculated via other correlations, more precise, accessible on Process Engineer's Tools website.
With :
Re = Reynolds number
The fluid velocity in the tubes depends on the number of tubes, the number of passes, the tube diameter and the mass flow of the fluid on the tube sides.
The number of tubes per pass can be calculated the following way :
Ntp = Nt/nt
The passing area of the fluid is then :
A = Ntp*(π.di2/4)
And the velocity is then :
V = (m/ρ)/A
With
Nt = number of tubes
nt = number of tube passes
Ntp = Number of tubes per pass
A = passing section of the fluid (m2)
ρ = density of the fluid (kg/m3)
V = fluid velocity in tubes (m/s)
m = mass flowrate of the fluid in the tube side (kg/s)
The total length of flow in the tubes is :
Lt = L*nt
With
Lt = total length of flow in tubes
L = length of tubes
nt = number of tube passes
The correction for non isothermal flow is due to Sieder and Tate and expressed as :
Φ = (μ/μw)-0.25 in laminar flow
Φ = (μ/μw)-0.14 in turbulent flow
With
μ = viscosity of the fluid at bulk temperature in Pa.s (kg/m/s)
μw = viscosity of the fluid at the wall temperature in
Pa.s (kg/m/s)
The pressure drop in the nozzles is calculated by :
ΔPi = 1.5*ρi*Vi2/2
ΔPo = 0.5*ρo*Vo2/2
With :
ΔPi = pressure drop in the inlet nozzle
ΔPo = pressure drop in the outlet nozzle
ρ = density of the fluid (kg/m3) with indice i for inlet and o for
outlet
V = fluid velocity in tubes (m/s) with indice i for inlet and o for
outlet
The pressure drop in the return cover depends on the fluid velocity and the number of passes. It can be calculated by :
ΔPc = (Ke.ρ.V2)/(2.nt)
With :
ΔPc = pressure drop in the return cover
Ke = coefficient dependent on the number of passes. 1st
approximation value is 0.9 for 1 tube pass and 1.6 for multi passes
tube
ρ = density of the fluid (kg/m3)
V = fluid velocity in tubes (m/s)
nt = number of tube passes