Frame of reference
- Define frame of reference, and notation. Use u,v,w and x,y, and z?
- Dumping a sketch would be useful
Reynold's Decomposition
- Variable names for Decomposition of total, mean, turbulent and waves.
Background (total) velocity
| Parameter name
|
Symbol
|
Description
|
Standard long name
|
Units
|
| EAST_VEL
|
<math> u </math>
|
zonal velocity
|
eastward_velocity
|
<math>\mathrm{m\, s^{-1}}</math>
|
| NORTH_VEL
|
<math> v </math>
|
meridional velocity
|
northward_velocity
|
<math>\mathrm{m\, s^{-1}}</math>
|
| UP_VEL
|
<math> W </math>
|
vertical velocity
|
upward_velocity
|
<math>\mathrm{m\, s^{-1}}</math>
|
| ERROR_VEL
|
<math> u_e </math>
|
error velocity
|
error_velocity
|
<math>\mathrm{m\, s^{-1}}</math>
|
| U_VEL
|
<math> U </math>
|
velocity parellel to mean flow
|
meanflow_velocity
|
<math>\mathrm{m\, s^{-1}}</math>
|
| V_VEL
|
<math> V </math>
|
velocity perpendicular to mean flow
|
crossflow_velocity
|
<math>\mathrm{m\, s^{-1}}</math>
|
| Drop_Speed
|
<math> W_d </math>
|
Profiler fall speed
|
mean_drop_speed
|
<math>\mathrm{m\, s^{-1}}</math>
|
| FlowPast_Speed
|
<math> U_P </math>
|
Flow speed past sensor
|
mean_velocity_past_turbulence_sensor
|
<math>\mathrm{m\, s^{-1}}</math>
|
| AlongBeam_Velocity
|
<math> b </math>
|
Along-beam velocity from acoustic Doppler sensor
|
observed_velocity_along_an_acoustic_beam
|
<math>\mathrm{m\, s^{-1}}</math>
|
| AlongBeam_Residual_Velocity
|
<math> b^{\prime} </math>
|
Along-beam velocity from acoustic Doppler sensor with background flow deducted
|
residual_velocity_along_an_acoustic_beam
|
<math>\mathrm{m\, s^{-1}}</math>
|
| Vertical_Bin_Size
|
<math> \delta{z} </math>
|
Vertical size of measurement bin for acoustic Doppler sensor
|
vertical_bin_size
|
<math>\mathrm{m}</math>
|
| AlongBeam_Distance
|
<math> r </math>
|
Along-beam distance from acoustic Doppler sensor
|
distance_along_an_acoustic_beam
|
<math>\mathrm{m}</math>
|
| AlongBeam_Bin_Size
|
<math> \delta{r} </math>
|
Along-beam bin size for acoustic Doppler sensor
|
bin_size_along_an_acoustic_beam
|
<math>\mathrm{m}</math>
|
| Beam_Angle
|
<math> \theta </math>
|
Beam transmit and receive angle relative to instrument axis for acoustic Doppler sensor
|
acoustic_beam_angle
|
<math> ^{\circ} </math>
|
Turbulence properties
| Parameter name
|
Symbol
|
Description
|
Standard long name
|
Eqn
|
Units
|
| EPSI
|
<math>\varepsilon</math>
|
Turbulent kinetic energy dissipation rate
|
tke_dissipation
|
|
<math> \mathrm{W\, kg^{-1}} </math>
|
| RI
|
<math>Ri</math>
|
Richardson number
|
richardson_number
|
<math> Ri = \frac{N^2}{S^2}</math>
|
|
| RI_F
|
<math>Ri_f</math>
|
Flux gradient Richardson number
|
flux_grad_richardson_number
|
<math> \frac{B}{P} </math> or Ivey & Immerger? Karan et cie
|
|
| Krho
|
<math>\kappa_\rho</math>
|
Turbulent diffusivity
|
turbulent_diffusivity
|
<math> \kappa = \Gamma \varepsilon N^{-2} </math>
|
<math>\mathrm{m^2\, s^{-1}}</math>
|
| DLL
|
<math>D_{LL}</math>
|
Second-order longitudinal structure function
|
second_order_longitudinal_structure_function
|
<math> D_{LL} = \big\langle[b^{\prime}(r) - b^{\prime}(r+n\delta{r})]^2\big\rangle </math>
|
<math>\mathrm{m^2\, s^{-2}}</math>
|
Fluid properties and background gradients for turbulence calculations
| Parameter Name
|
Symbol
|
Description
|
Standard long name
|
Eqn
|
Units
|
| Z
|
<math>z</math>
|
vertical coordinate -- positive upwards
|
vertical_coordinate
|
|
<math>\mathrm{m} </math>
|
| G
|
<math>g</math>
|
acceleration of gravity
|
acceleration_of_gravity
|
<math> \sim 9.81 </math>
|
<math>\mathrm{m\, s^{-2}} </math>
|
| SALINITY
|
<math>S_a</math>
|
Salinity
|
Salinity
|
<math> \sim 35 </math>
|
|
| TEMP
|
<math>T</math>
|
Temperature
|
Temperature
|
<math> \sim -2 \rightarrow 40 </math>
|
<math> \mathrm{^{\circ}C } </math>
|
| PRES
|
<math>P</math>
|
Pressure
|
Pressure
|
<math> 0\ \rightarrow\ \sim 1\times10^4 </math>
|
<math> \mathrm{dbar} </math>
|
| DENSITY
|
<math>\rho</math>
|
Density of water
|
Density
|
<math> \rho = \rho\left(T,S_a,P \right) </math>
|
<math> \mathrm{kg\, m^{-3}} </math>
|
| ALPHA
|
<math>\alpha</math>
|
Temperature coefficient of expansion
|
Temperature_coefficient_of_expansion
|
<math> \alpha = \frac{1}{\rho} \frac{\partial\rho}{\partial T} </math>
|
<math> \mathrm{K^{-1}} </math>
|
| BETA
|
<math>\beta</math>
|
Saline coefficient of contraction
|
Saline_coefficient_of_contraction
|
<math> \beta = \frac{1}{\rho} \frac{\partial\rho}{\partial S_a} </math>
|
<math> </math>
|
| S
|
<math>S</math>
|
Background velocity shear
|
background_velocity_shear
|
<math> S = \left( \left( \frac{\partial U}{\partial z}\right)^2 + \left( \frac{\partial V}{\partial z}\right)^2 \right)^{1/2}</math>
|
s<math>^{-1}</math>
|
| KVISC35
|
<math>\nu_{35}</math>
|
Temperature dependent kinematic viscosity of seawater at a salinity of 35
|
seawater_kinematic_viscosity_at_35psu
|
<math> \sim 1\times 10^{-6}</math>
|
<math> \mathrm{m^2\, s^{-1} } </math>
|
| KVISC00
|
<math>\nu_{00}</math>
|
Temperature dependent kinematic viscosity of freshwater
|
freshwater_kinematic_viscosity
|
<math> \sim 1\times 10^{-6}</math>
|
<math> \mathrm{m^2\, s^{-1} } </math>
|
| GAMMA_A
|
<math>\Gamma</math>
|
Adiabatic temperature gradient -- salinity, temperature and pressure dependent
|
Rate of change of temperature due to pressure
|
<math> \sim 1\times 10^{-4} </math>
|
<math> \mathrm{K\, dbar^{-1} } </math>
|
| N
|
<math>N</math>
|
Background stratification, i.e buoyancy frequency
|
background_buoyancy_frequency
|
<math> N^2 = g\left[ \alpha\left(\Gamma + \frac{\partial T}{\partial z} \right) - \beta \frac{\partial S_a}{\partial z} \right] </math>
|
<math> \mathrm{rad\, s^{-1} } </math>
|
Theoretical Length and Time Scales
| Parameter
|
Symbol
|
Description
|
Standard long name
|
Eqn
|
Units
|
| T_N
|
<math>\tau_N</math>
|
Buoyancy timescale
|
buoyancy_time_scale
|
<math> \tau_N = \frac{2\pi}{N}</math>
|
s
|
| L_E
|
<math>L_E</math>
|
Ellison length scale (limit of vertical displacement without irreversible mixing)
|
Eliison_lenght_scale
|
<math>L_E=\frac {\langle \rho'^2\rangle^{1/2}}{\partial \overline{\rho}/\partial z}</math>
|
m
|
| L_RHO
|
<math> L_\rho</math>
|
Density length scale
|
density_length_scale
|
<math> L_\rho </math>
|
m
|
| L_S
|
<math>L_S</math>
|
Corssin length scale
|
Corssin_shear_length_scale
|
<math> L_S = \sqrt{\varepsilon/S^3} </math>
|
m
|
| L_K
|
<math>\eta</math>
|
Kolmogorov length scale (smallest overturns)
|
Kolmogorov_length_scale
|
<math>\eta=\left(\frac{\nu^3}{\varepsilon}\right)^{1/4}=\frac{1}{2\pi\hat{k}_K}</math>
|
m
|
| L_O
|
<math>L_o</math>
|
Ozmidov length scale, measure of largest overturns in a stratified fluid
|
Ozmidov_stratification_length_scale
|
<math>L_o=\left(\frac{\varepsilon}{N^3}\right)^{1/2}</math>
|
m
|
| L_T
|
<math>L_T</math>
|
Thorp length scale
|
Thorpe_stratification_length_scale
|
<math>L_T</math>
|
m
|
Turbulence Spectrum
Taylor's Frozen Turbulence for converting temporal to spatial measurements <math>\left(\bar{u}_1\frac{\partial
}{\partial{x}} = \frac{\partial}{\partial{t}}\right)</math>
- Missing the y-axi variable. CEB proposes:
- <math>\Psi_{variable}</math> for model/theoretical spectrum of variable e.g., du/dx or u
- <math>\Phi_{variable}</math> for observed spectrum of variable e.g., du/dx or u
- Lowest frequency and wavenumber resolvable
| Symbol
|
Description
|
Eqn
|
Units
|
| <math>\Delta t</math>
|
Sampling interval
|
<math> \frac{1}{f_s} </math>
|
<math> \mathrm{s} </math>
|
| <math>f_s</math>
|
Sampling rate
|
<math>f_s=\frac{1}{\Delta t} </math>
|
<math> \mathrm{s^{-1}} </math>
|
| <math>\Delta s</math>
|
Sampling volume dimension
|
<math> \Delta s = U_P \Delta t </math>
|
<math> \mathrm{m} </math>
|
| <math>f</math>
|
Cyclic frequency
|
<math>f=\frac{\omega}{2\pi}</math>
|
<math> \mathrm{Hz} </math>
|
| <math>\omega</math>
|
Angular frequency
|
<math>\omega = 2\pi f</math>
|
<math> \mathrm{rad\, s^{-1}} </math>
|
| <math>f_N</math>
|
Nyquist frequency
|
<math>f_N=0.5f_s</math>
|
<math> \mathrm{Hz} </math>
|
| <math>k</math>
|
Wavenumbers (angular)
|
<math>k=\frac{f}{\bar{u}}=2\pi\hat{k}</math>
|
rad/m
|
| <math>\hat{k}</math>
|
Wavenumbers
|
<math>\hat{k}=\frac{k}{2\pi}</math>
|
cpm
|
| <math>\hat{k}_\Delta</math>
|
Nyquist wavenumber, based on sampling volume's size <math>\Delta l</math>
|
<math>\hat{k}_\Delta=\frac{0.5}{\Delta l}</math>
|
cpm
|
| <math>\hat{k}_n</math>
|
Nyquist wavenumber, via Taylor's hypothesis (temporal measurements)
|
<math>\hat{k}_n=\frac{f_n}{u}</math>
|
cpm
|
| <math>\omega</math>
|
Angular frequency
|
<math>2\pi f</math>
|
rad/s
|
Supplementary Data required for computing Turbulence
| Channel |
Shear Probes |
ADCP |
ADVs
|
| Ax |
x |
x |
x
|
| Ay |
x |
x |
x
|
| Az |
x |
x |
x
|