Upload
zain-ulabideen
View
215
Download
0
Embed Size (px)
DESCRIPTION
DN
Citation preview
ARCHIMEDES NUMBER is proportional to { (gravitational force) / (viscous force) } and is used in momentum transfer in general and buoyancy, fluidization, and motion due to density
difference calculations in particular. It is normally defined in the following form :
Where:
g = Gravitational acceleration
L = Characteristic length
mu = Viscosity
rho_f = Fluid density
rho_s = Solid density
Arrhenius number is proportional to { (activation energy) / (potential energy) } and is used in
mass transfer in general and reaction rate calculations in particular. It is normally defined in the
following form
Where:
Eo = Activation Energy
R = Gas law constant
T = Temperature
Bingham number is proportional to { (yield stress) / (viscous stress) } and is used in momentum
transfer in general and flow of bingham plastics calculations in particular. It is normally defined
in the following form :
Where:
gc = Dimensional constant
L = Characteristic length
mu = Viscosity
tau_y = Stress
V = Velocity
Biot number is proportional to { (thermal internal resistance) / (surface film resistance) } and is
used in heat transfer in general and unsteady state calculations in particular. It is normally
defined in the following form :
Where:
delta-x = Mid-plane distance
h_T = Heat transfer coefficient
k = Thermal Conductivity
Blake number is proportional to { (inertial force) / (viscous force) } and is used in momentum
transfer in general and flow through beds of solids calculations in particular. It is normally
defined in one of the following forms :
or
Where:
epsilon = Void fraction
G = Mass velocity
mu = Viscosity
rho = Density
s = Particle area/particle volume
V = Velocity
Bodenstein number is used in mass transfer in general and diffusion in reactors calculations in
particular. It is normally defined in the following form :
Where:
Dv,a = Effective axial diffusivity
L = Reactor length
V = Velocity
Where:
d = Droplet/bubble diameter
g = Gravitational acceleration
gc = Dimensional constant
rho = Droplet/bubble density
rho_f = Surrounding fluid density
sigma = Surface tension
Capillary number is proportional to { (viscous force) / (surface tension force) } and is used in
momentum transfer in general and atomization and 2-phase flow in beds of solids calculations in
particular. It is equivalent to (We/Re). It is normally defined in the following form
Where:
gc = Dimensional constant
mu = Viscosity
sigma = Surface tension
V = Velocity
Cauchy number is proportional to { (inertial force) / (compressibility force) } and is used in
momentum transfer in general and compressible flow calculations in particular. It is normally
defined in the following form :
Where:
Eb = bulk modulus of fluid
gc = Dimensional constant
rho = Density
V = Velocity
Cavitation number is proportional to { (excess of local static head over vapor pressure head) /
(velocity head) } and is used in momentum transfer in general and throttling calculations in
particular. It is normally defined in the following form :
Where:
gc = Dimensional constant
p = Local static pressure
p_v = Vapor pressure
rho = Density
V = Velocity
Colburn-Chilton j factor is used in heat transfer in general and free and forced convection
calculations in particular. It is equivalent to (St.Pr^2/3). It is normally defined in one of the
following forms :
or
Where:
Cp = Heat capacity
G = Mass velocity
h = Heat transfer coefficient
k = Thermal Conductivity
mu = Viscosity
rho = Density
V = Velocity
Condensation number is used in heat transfer in general and as the name implies in condensation
calculations in particular. It is normally defined in one of the following forms :
or
Where:
delta-T = Temperature difference
lambda = Latent heat
g = Gravitational
acceleration
h = Heat transfer coefficient
k = Thermal Conductivity
L = Characteristic length
mu = Viscosity
rho = Density
Drag Coefficient
Drag coefficient is proportional to { (gravitational force) / (inertial force) } and is used in
momentum transfer in general and free settling velocities and resistance to flow calculations in
particular. It is normally defined in the following form :
Where:
g = Gravitational acceleration
L = Characteristic dimension of object
rho = Density of object
rho_f = Density of surrounding fluid
V = Velocity
Eckert Number
Eckert number is used in momentum and heat transfer in general and compressible flow
calculations in particular. It is normally defined in the following form :
Where:
Cp = Heat capacity
delta-T = Temperature difference
V_inf = Velocity of fluid far from body
Elasticity Number
Elasticity number is proportional to { (elastic force) / (inertial force) } and is used in momentum
transfer in general and viscoelastic flow calculations in particular. It is normally defined in the
following form :
Where:
r = Pipe/conduit radius
mu = Viscosity
rho = Density
theta = relaxation time
Etvs number is proportional to { (gravitational force) / (surface tension force) } and is used in
momentum transfer in general and atomization, and motion of bubbles and droplets calculations
in particular. It is equivalent to (Bo). It is normally defined in the following form :
Where:
L = Characteristic length
rho = Density of
bubble/droplet
rho_f = Density of surrounding fluid
sigma = Surface tension
Euler Number
Euler number is proportional to { (friction head) * (velocity head) } and is used in momentum
transfer in general and fluid friction in conduits calculations in particular. It is equivalent to (N/2)
where N is the number of velocity heads. It is normally defined in one of the following forms :
or
Where:
delta-P = Pressure drop
gc = Dimensional constant
G = Mass velocity
rho = Density
V = Velocity
Fourier Number
Fourier number is used in heat transfer in general and unsteady state heat transfer calculations in
particular. It is normally defined in one of the following forms :
or
Where:
alpha = Thermal diffusivity
Cp = Heat capacity
k = Thermal Conductivity
L = Characteristic length
rho = Density
t = Time
Froude Number
Froude number is proportional to { (inertial force) / (gravitational force) } and is used in
momentum transfer in general and open channel flow and wave and surface behavior
calculations in particular. It is normally defined in one of the following forms
or
Where:
a = Acceleration
g = Gravitational acceleration
L = Characteristic length
V = Velocity
Galileo Number
Galileo number is proportional to { (Re. gravity force) / (viscous force) } and is used in
momentum and heat transfer in general and viscous flow and thermal expansion calculations in
particular. It is normally defined in the following form :
Where:
g = Gravitational acceleration
D = Diameter
mu = Viscosity
rho = Density
Grtz Number
Grtz number is proportional to { (thermal capacity) / (convective heat transfer) } and is used in
heat transfer in general and convection in laminar flow calculations in particular. It is equivalent
to {(L/d) / (Re.Pr)} or {(L/d) / Pe}. It is normally defined in one of the following forms :
Where:
alpha = Thermal diffusivity
Cp = Heat capacity
d = Diameter
G = Mass velocity
k = Thermal Conductivity
L = Length
m = Mass flowrate
rho = Density
V = Velocity
Grashof Number
Grashof number is proportional to { (buoyancy force) / (viscous force) } and is used in heat
transfer in general and free convection calculations in particular. It is normally defined in one of
the following forms :
or
Where:
beta = Coefficient of expansion
delta-T = Temperature difference
G = Gravitational acceleration
L = Characteristic length
mu = Viscosity
V = Kinematic viscosity
rho = Density
Hodgson Number
Hodgson number is proportional to { (time constant of system) / (period of pulsation) } and is
used in momentum transfer in general and unsteady pulsating gas flow calculations in particular.
It is normally defined in the following form :
Where:
delta-P = Pressure drop
fr = Frequency
p = Avg. static pressure
q = Avg. volumetric flowrate
V = System Volume
Knudsen Number
Knudsen number is proportional to { (length of mean free path) / (characteristic dimension) }
and is used in momentum and mass transfer in general and very low pressure gas flow
calculations in particular. It is normally defined in the following form :
Where:
lambda = Length of mean free path
L = Characteristic dimension
Lewis Number
Lewis number is used in combined heat and mass transfer calculations. It is equivalent to (Sc/Pr).
It is normally defined in one of the following forms :
or
Where:
alpha = Thermal diffusivity
Cp = Heat capacity
Dv = Diffusivity
k = Thermal Conductivity
rho = Density
Mach number is used in momentum transfer in general and near/ultra sonic flow and throttling
calculations in particular. It is normally defined in the following form :
Where:
V = Velocity
V_sound = Velocity of sound in fluid
Nusselt Number
Nusselt number is proportional to { (total heat transfer) / (conductive heat transfer) } and is used
in heat transfer in general and forced convection calculations in particular. It is normally defined
in the following form :
Where:
h = Heat transfer coefficient
D = Diameter
k = Thermal Conductivity
Ohnesorge Number
Ohnesorge number is proportional to { (viscous force) / (sqrt (inertial force . surface tension
force)) } and is used in momentum transfer in general and atomization calculations in particular.
It is equivalent to (SQRT(We) / Re). It is normally defined in the following form :
Where:
gc = Dimensional constant
L = Characteristic length
mu = Viscosity
rho = Density
sigma = Surface tension
Peclet Number
Peclet number is proportional to { (bulk heat transfer) / (conductive heat transfer) } and is used
in heat transfer in general and forced convection calculations in particular. It is equivalent to
(Re.Pr). It is normally defined in one of the following forms :
or
Where:
alpha = Thermal diffusivity
Cp = Heat capacity
D = Characteristic length
G = Mass velocity
k = Thermal Conductivity
rho = Density
V = Velocity
Pipeline Parameter
Pipeline parameter is proportional to { (maximum water-hammer pressure rise) / (2 static
pressure) } and is used in momentum transfer in general and hydraulic transients calculations in
particular. It is normally defined in the following form :
Where:
a = Wave velocity
g = Gravitational acceleration
H = Static head
Vo = Initial velocity
Power Number
Power number is proportional to { (drag force) / (inertial force) } and is used in momentum
transfer in general and power consumption by agitators, fans, pumps, etc. calculations in
particular. It is normally defined in the following form :
Where:
D = Characteristic length
gc = Dimensional constant
N = Rate of rotation
P = Power
rho = Density
Prandtl Number
Prandtl number is proportional to { (momentum diffusivity) / (thermal diffusivity) } and is used
in heat transfer in general and free and forced convection calculations in particular. It is normally
defined in the following form :
Where:
Cp = Heat capacity
k = Thermal Conductivity
mu = Viscosity
Rayleigh Number
Rayleigh number is used in heat transfer in general and free convection calculations in particular.
It is equivalent to (Gr.Pr). It is normally defined in one of the following forms :
or
Where:
alpha = Thermal diffusivity
beta = Coefficient of expansion
Cp = Heat capacity
delta-T = Temperature difference
g = Gravitational acceleration
k = Thermal Conductivity
L = Characteristic length
mu = Viscosity
rho = Density
Reynolds Number
Reynolds number is proportional to { (inertial force) / (viscous force) } and is used in
momentum, heat, and mass transfer to account for dynamic similarity. It is normally defined in
one of the following forms
For Reynolds Number Calculation using the above formula please go Here
http://www.processassociates.com/reynolds.php
or
Where:
D = Characteristic length
G = Mass velocity
mu = Viscosity
rho = Density
V = Velocity
Schmidt Number
Schmidt number is proportional to { (kinetic viscosity) / (molecular diffusivity) } and is used in
mass transfer in general and diffusion in flowing systems calculations in particular. It is normally
defined in the following form :
Where:
Dv = Diffusivity
mu = Viscosity
rho = Density
Sherwood Number
Sherwood number is proportional to { (massr diffusivity) / (molecular diffusivity) } and is used
in mass transfer calculations. It is equivalent to (jm.Re.Sc1/3). It is normally defined in the
following form :
Where:
Dv = Diffusivity
kc = Diffusion rate
L = Characteristic length
Stanton Number
Stanton number is proportional to { (heat transfered) / (thermal capacity of fluid) } and is used in
heat transfer in general and forced convection calculations in particular. It is equivalent to (Nu /
(Re.Pr)). It is normally defined in one of the following forms :
or
Where:
Cp = Heat capacity
G = Mass velocity
h = Heat transfer coefficient
rho = Density
V = Velocity
Strouhal Number
Strouhal number is proportional to the reciprocal of vortex spacing expressed as no. of obstacle
diameters and is used in momentum transfer in general and Van Karman vortex streets and
unsteady state flow calculations in particular. It is normally defined in the following form :
Where:
fr = frequency
L = Characteristic length
V = Velocity
Weber Number
Weber number is proportional to { (inertial force) / (surface tension force) } and is used in
momentum transfer in general and bubble/droplet formation and breakage of liquid jets
calculations in particular. It is normally defined in one of the following forms :
or
Where:
gc = Dimensional constant
G = Mass velocity
D = Characteristic length
rho = Density
sigma = Surface tension
V = Velocity