Ice Adhesion. Группа авторов

Ice Adhesion - Группа авторов


Скачать книгу
viscosity. Note that Prandtl’s number for air at -20°C is 0.75. Considering ice growth, a quasi-steady process, by energy balance at water-ice interface Eq. (3.23) can be obtained in this case as well. Due to the radial ice growth, the velocity of freezing front is written as Eq. (3.30).

      Where Ai is ice-water interface area and Ao is ice-air interface area. By substituting Eq. (3.23) and (3.30) in Eq. (3.31), the following equation is obtained,

      (3.32)c03_Inline_15_16.jpg

      Now, we can find an equation for ice growth rate. Through solution of heat equation in spherical coordinates, we have,

      (3.33)c03_Inline_15_17.jpg

      T(r = ri) = Tf and T(r = r0) = Ts are ice-water and ice-air interface temperatures, respectively. The boundary conditions are written as,

c03_Inline_15_19.jpg c03_Inline_15_20.jpg c03_Inline_16_11.jpg

      We define,

c03_Inline_16_12.jpg

      Thus,

      (3.35)c03_Inline_16_13.jpg

      (3.36)c03_Inline_16_14.jpg

      The surface temperature is as follows:

c03_Inline_16_15.jpg

      where c03_Inline_16_16.jpg and θs = TsT. By substitution of C1 and C2, the following equation for θs is obtained:

c03_Inline_17_12.jpg

      Thus, c03_Inline_17_18.jpg is written as:

c03_Inline_17_13.jpg

      And c03_Inline_17_19.jpg may be simplified to

      Where Biot number is defined as:

c03_Inline_17_15.jpg

      By writing the energy balance at the ice-water interface one has:

      (3.38)c03_Inline_17_16.jpg

c03_Inline_18_13.jpg

      And by simplification of this equation, one finds

c03_Inline_18_14.jpg

      Through integration of both sides:

c03_Inline_18_15.jpg

      And we have the initial condition for ice growth as:

c03_Inline_18_16.jpg

      Thus,

      A critical factor in ice growth in airflow is humidity. For example, in the presence of airflow, at humidity of 30-75%, ice nucleation occurs at liquid-vapor interface which is called homogeneous nucleation, while at humidity close to 100%, heterogeneous ice nucleation which is ice nucleation at solid-liquid interface occurs [24]. This phenomenon can be justified by evaporation rate. Evaporation rate is higher at lower humidity. Therefore, at lower humidity high rate of evaporation cools down the liquid-vapor interface leading to ice nucleation at this interface. On the other hand, once evaporation rate is low in high humidity, ice nucleation occurs at solid-liquid interface. Note that humidity also affects ice growth in the environments with airflow. Airflow with higher amount of humidity


Скачать книгу