Nomenclature: Difference between revisions
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| <math> \sim -2 \rightarrow 40 </math> | | <math> \sim -2 \rightarrow 40 </math> | ||
| <math> \mathrm{^{\circ}C } </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 | | S | ||
Revision as of 18:23, 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
| Symbol | Description | Eqn | Units |
|---|---|---|---|
| <math>\Delta t</math> | Sampling interval | <math> \frac{1}{f_s} </math> | s |
| <math>\Delta s</math> | Sampling volume dimension | m | |
| <math>f</math> | Frequency | <math>\frac{\omega}{2\pi}</math> | Hz |
| <math>f_n</math> | Nyquist frequency | <math>f_n=0.5f_s</math> | Hz |
| <math>f_s</math> | Sampling frequency | <math>f_s=\frac{1}{\Delta t} </math> | Hz |
| <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 |
