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Difference between revisions of "Anemometer"

Line 18: Line 18:
   
 
<math>\rho c \frac{\partial T}{\partial t} = \nabla \cdot (\kappa
 
<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 \nabla T + \dot q,</math>
   
 
where <math>\rho</math> denotes the mass density, <math>c</math> is the specific heat,
 
where <math>\rho</math> denotes the mass density, <math>c</math> is the specific heat,

Revision as of 17:17, 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]:

\rho c \frac{\partial T}{\partial t} = \nabla \cdot (\kappa
  \nabla T ) - \rho c v \nabla T + \dot q,

where \rho denotes the mass density, c is the specific heat, \kappa is the thermal conductivity, v is the fluid velocity, T is the temperature and \dot q the heat flow into the system caused by the heater.