Now we show the graph of the
inversely proportional relation between flow and viscosity.

Letting all of the parameters except the viscosity remain at the
standard values, choose the viscosity that you want to consider.
You can determine the value of the flow geometrically by finding
your viscosity value on
the horizontal axis (independent variable), finding the point on the graph directly
above this number, and then reading the value of the number directly to the left of this
point (dependent variable).
The shape of this graph is called a hyperbola. Notice that as the viscosity
gets larger (moving to the right), the value of the flow becomes smaller.
If the viscosity gets arbitrarily large, then the flow vanishes. This is
referred to as a horizontal asymptote of Q=0. Also, as the viscosity gets
smaller the flow increases without bound (in the graph). This corresponds to
a vertical asymptote at n=0. However, this does not mean that the physical
situation can actually sustain arbitrarily large flow. When the viscosity
becomes too small, then turbulence begins and the model no longer applies.