We need to find the total charge enclosed in a cylindrical volume with a given charge density. The charge density is given as a function of the radial coordinate \( r \) in cylindrical coordinates: \(\rho(r) = 3r + r^3\). The volume of interest is defined by the region \(0 \leq r \leq 1\), \(0 \leq z \leq 1\), and \(0 \leq \theta \leq 2\pi\).
The total charge \( Q \) enclosed in the volume can be found by integrating the charge density over the specified volume. The differential volume element in cylindrical coordinates is given by \( dV = r \, dz \, dr \, d\theta \).
The integral to find the total charge is:
\[
Q = \int_0^{2\pi} \int_0^1 \int_0^1 \rho(r) \, r \, dz \, dr \, d\theta
\]
Substitute \(\rho(r) = 3r + r^3\) into the integral:
\[
Q = \int_0^{2\pi} \int_0^1 \int_0^1 (3r + r^3) \, r \, dz \, dr \, d\theta
\]
Simplify the integrand:
\[
Q = \int_0^{2\pi} \int_0^1 \int_0^1 (3r^2 + r^4) \, dz \, dr \, d\theta
\]
First, integrate with respect to \( z \):
\[
Q = \int_0^{2\pi} \int_0^1 (3r^2 + r^4) \, [z]_0^1 \, dr \, d\theta = \int_0^{2\pi} \int_0^1 (3r^2 + r^4) \, dr \, d\theta
\]
Next, integrate with respect to \( r \):
\[
Q = \int_0^{2\pi} \left[ \frac{3r^3}{3} + \frac{r^5}{5} \right]_0^1 \, d\theta = \int_0^{2\pi} \left( r^3 + \frac{r^5}{5} \right)_0^1 \, d\theta
\]
\[
= \int_0^{2\pi} \left( 1 + \frac{1}{5} \right) \, d\theta = \int_0^{2\pi} \frac{6}{5} \, d\theta
\]
Finally, integrate with respect to \( \theta \):
\[
Q = \left[ \frac{6}{5} \theta \right]_0^{2\pi} = \frac{6}{5} \times 2\pi = \frac{12\pi}{5}
\]
The total charge enclosed in the specified volume is \(\boxed{\frac{12\pi}{5}}\).