Step 1: Understand the velocity profile for fully developed laminar flow in a circular tube.
For fully developed laminar flow through a circular tube, the velocity profile is parabolic. The velocity is maximum at the center of the tube and zero at the tube walls due to the no-slip condition.
The velocity profile \( u(r) \) at a radial distance \( r \) from the center of the pipe is given by:
\[
u(r) = -\frac{1}{4\mu} \left(\frac{dP}{dx}\right) (R^2 - r^2)
\]
where:
\( \mu \) = dynamic viscosity of the fluid
\( \frac{dP}{dx} \) = pressure gradient along the pipe
\( R \) = radius of the pipe
\( r \) = radial distance from the center
Step 2: Determine the maximum velocity.
The maximum velocity, \( u_{max} \), occurs at the center of the pipe where \( r=0 \).
\[
u_{max} = -\frac{1}{4\mu} \left(\frac{dP}{dx}\right) R^2
\]
Step 3: Determine the average velocity.
The average velocity, \( u_{avg} \), for fully developed laminar flow in a circular tube can be found by integrating the velocity profile over the cross-sectional area and dividing by the area, or by using the relationship from Hagen-Poiseuille equation.
It is a standard result that for a parabolic velocity profile, the average velocity is exactly half of the maximum velocity.
\[
u_{avg} = \frac{1}{2} u_{max}
\]
To verify this, the average velocity can be calculated as:
\[
u_{avg} = \frac{\int_0^R u(r) (2\pi r) dr}{\pi R^2}
\]
Substituting \( u(r) \) and performing the integration, we indeed find \( u_{avg} = \frac{1}{8\mu} \left(-\frac{dP}{dx}\right) R^2 \).
Comparing this to \( u_{max} = \frac{1}{4\mu} \left(-\frac{dP}{dx}\right) R^2 \), we get:
\( u_{avg} = \frac{1}{2} u_{max} \).
Step 4: Calculate the ratio of maximum velocity to average velocity.
\[
\frac{u_{max}}{u_{avg}} = \frac{u_{max}}{\frac{1}{2} u_{max}} = 2
\]
So, the ratio of maximum velocity to average velocity for fully developed laminar viscous flow through a circular tube is 2.0.
The final answer is $\boxed{\text{3}}$.