Nomenclature: Difference between revisions

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|-
|-
| <math>\Delta s</math>
| <math>\Delta s</math>
| Sampling volume dimension
| Sample spacing
| <math> \Delta s = U_P \Delta t </math>
| <math> \Delta s = U_P \Delta t </math>
| <math> \mathrm{m} </math>
|-
| <math>\Delta l</math>
| Linear dimension of sampling volume (instrument dependent)
|
| <math> \mathrm{m} </math>
| <math> \mathrm{m} </math>
|-
|-
Line 370: Line 375:
| Angular wavenumber
| Angular wavenumber
| <math>\hat{k}=\frac{\omega}{U_P} = 2\pi k</math>
| <math>\hat{k}=\frac{\omega}{U_P} = 2\pi k</math>
| <math> \mathrm{rad\, m^{-1}} </math>
|-
| <math>k_\Delta</math>
| Nyquist wavenumber, based on sampling volume size <math>\Delta l</math>
| <math>k_\Delta=\frac{0.5}{\Delta l}</math>
| <math> \mathrm{cpm} </math>
| <math> \mathrm{cpm} </math>
|-
|-
| <math>\hat{k}_\Delta</math>
| <math>k_N</math>
| Nyquist wavenumber, based on sampling volume's size <math>\Delta l</math>
| Nyquist wavenumber, via Taylor's hypothesis
| <math>\hat{k}_\Delta=\frac{0.5}{\Delta l}</math>
| <math>k_N=\frac{f_N}{U_P}</math>
| <math> \mathrm{cpm} </math>
| <math> \mathrm{cpm} </math>
|-
|-
| <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 ==
== Supplementary Data required for computing Turbulence ==

Revision as of 18:50, 23 April 2021

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
}

Supplementary Data required for computing Turbulence

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> Sample spacing <math> \Delta s = U_P \Delta t </math> <math> \mathrm{m} </math>
<math>\Delta l</math> Linear dimension of sampling volume (instrument dependent) <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> Cyclic wavenumber <math>k=\frac{f}{U_P}</math> <math> \mathrm{cpm} </math>
<math>\hat{k}</math> Angular wavenumber <math>\hat{k}=\frac{\omega}{U_P} = 2\pi k</math> <math> \mathrm{rad\, m^{-1}} </math>
<math>k_\Delta</math> Nyquist wavenumber, based on sampling volume size <math>\Delta l</math> <math>k_\Delta=\frac{0.5}{\Delta l}</math> <math> \mathrm{cpm} </math>
<math>k_N</math> Nyquist wavenumber, via Taylor's hypothesis <math>k_N=\frac{f_N}{U_P}</math> <math> \mathrm{cpm} </math>
Channel Shear Probes ADCP ADVs
Ax x x x
Ay x x x
Az x x x