We now wish to let the mass transfer rate vary in time. Choosing a single frequency may not be completely realistic, but it is simple and will show the effect.
Note that a mass transfer coefficient never is negative so we need something a little more complex than a sine wave. Here we have a background minimum value of ka, a frequency ω and a maximum value, kb.
![[Graphics:../Images/reactor_gr_55.gif]](../Images/reactor_gr_55.gif)
![[Graphics:../Images/reactor_gr_56.gif]](../Images/reactor_gr_56.gif)
![[Graphics:../Images/reactor_gr_57.gif]](../Images/reactor_gr_57.gif)
Here we change the values.
![[Graphics:../Images/reactor_gr_58.gif]](../Images/reactor_gr_58.gif)
![[Graphics:../Images/reactor_gr_59.gif]](../Images/reactor_gr_59.gif)
This seems to work well for the mass transfer coefficient. We can now just incorporate it into the model we have been using.
![[Graphics:../Images/reactor_gr_60.gif]](../Images/reactor_gr_60.gif)
![[Graphics:../Images/reactor_gr_62.gif]](../Images/reactor_gr_62.gif)
![[Graphics:../Images/reactor_gr_64.gif]](../Images/reactor_gr_64.gif)
![[Graphics:../Images/reactor_gr_66.gif]](../Images/reactor_gr_66.gif)
![[Graphics:../Images/reactor_gr_68.gif]](../Images/reactor_gr_68.gif)
![[Graphics:../Images/reactor_gr_70.gif]](../Images/reactor_gr_70.gif)
![[Graphics:../Images/reactor_gr_72.gif]](../Images/reactor_gr_72.gif)
![[Graphics:../Images/reactor_gr_74.gif]](../Images/reactor_gr_74.gif)