Step 1: Understanding the Problem
The mass of a small element of the rod at a distance \( x \) from one end is given by:
\[
dm = \rho(x) \, dx = \rho_0 \frac{x^2}{L^2} \, dx
\]
The position of the center of mass is given by the formula:
\[
x_{\text{cm}} = \frac{\int_0^L x \, dm}{\int_0^L dm}
\]
Where:
- The numerator is the first moment of mass,
- The denominator is the total mass of the rod.
Step 2: Total Mass of the Rod
The total mass \( M \) of the rod is obtained by integrating the mass element \( dm \) over the length of the rod:
\[
M = \int_0^L \rho(x) \, dx = \int_0^L \rho_0 \frac{x^2}{L^2} \, dx = \rho_0 \frac{1}{L^2} \int_0^L x^2 \, dx
\]
The integral of \( x^2 \) from 0 to \( L \) is:
\[
\int_0^L x^2 \, dx = \frac{L^3}{3}
\]
Thus:
\[
M = \rho_0 \frac{1}{L^2} \cdot \frac{L^3}{3} = \frac{\rho_0 L}{3}
\]
Step 3: First Moment of Mass
The first moment of mass is:
\[
\int_0^L x \, dm = \int_0^L x \rho_0 \frac{x^2}{L^2} \, dx = \rho_0 \frac{1}{L^2} \int_0^L x^3 \, dx
\]
The integral of \( x^3 \) from 0 to \( L \) is:
\[
\int_0^L x^3 \, dx = \frac{L^4}{4}
\]
Thus:
\[
\int_0^L x \, dm = \rho_0 \frac{1}{L^2} \cdot \frac{L^4}{4} = \frac{\rho_0 L^2}{4}
\]
Step 4: Position of the Center of Mass
Now we can calculate the position of the center of mass:
\[
x_{\text{cm}} = \frac{\frac{\rho_0 L^2}{4}}{\frac{\rho_0 L}{3}} = \frac{3L}{4}
\]
Step 5: Conclusion
The position of the center of mass from one end is \( \frac{3L}{4} \).
Thus, the correct answer is:
\[
\boxed{(D)} \, \frac{3L}{4}
\]