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The physical model can be expressed by the |
The physical model can be expressed by the |
||
| − | convection-diffusion partial differential equation |
+ | convection-diffusion partial differential equation[4]: |
| − | <math> |
+ | <math>\rho c \frac{\partial T}{\partial t} = \nabla \cdot (\kappa |
\nabla T ) - \rho c v \normalfont \nabla T + \dot q,</math> |
\nabla T ) - \rho c v \normalfont \nabla T + \dot q,</math> |
||
Revision as of 17:16, 28 November 2011
Description
An anemometer, a flow sensing device, consists of a heater and temperature sensors before and after the heater, placed either directly in the flow or in its vicinity. They are located on a membrane to minimize heat dissipation through the structure. Without any flow, the heat dissipates symmetrically into the fluid. This symmetry is disturbed if a flow is applied to the fluid, which leads to a convection on the temperature field and therefore to a difference between the temperature sensors (see Fig.1 below) from which the fluid velocity can be determined.
The physical model can be expressed by the convection-diffusion partial differential equation[4]:
Failed to parse (unknown function "\normalfont"): \rho c \frac{\partial T}{\partial t} = \nabla \cdot (\kappa \nabla T ) - \rho c v \normalfont \nabla T + \dot q,
where 
denotes the mass density, 
is the specific heat,
is the thermal conductivity, 
is the fluid
velocity, 
is the temperature and 
the heat flow into the system
caused by the heater.