We are given a rod of length \( L \), with a linear mass density that varies along the length of the rod. The linear mass density \( \lambda(x) \) at a point at a distance \( x \) from the left end of the rod is given by:
\[
\lambda(x) = 2x \, \text{kg/m}
\]
The center of mass \( x_{\text{cm}} \) of the rod can be found using the following formula:
\[
x_{\text{cm}} = \frac{\int_0^L x \, \lambda(x) \, dx}{\int_0^L \lambda(x) \, dx}
\]
First, we calculate the mass of the rod using the linear mass density. The total mass \( M \) of the rod is given by the integral of \( \lambda(x) \) over the length of the rod:
\[
M = \int_0^L \lambda(x) \, dx = \int_0^L 2x \, dx
\]
Performing the integration:
\[
M = \left[ x^2 \right]_0^L = L^2
\]
Thus, the total mass of the rod is \( M = L^2 \, \text{kg} \).
Now, we calculate the moment of mass distribution about the left end of the rod:
\[
\int_0^L x \, \lambda(x) \, dx = \int_0^L x \cdot 2x \, dx = 2 \int_0^L x^2 \, dx
\]
Performing the integration:
\[
\int_0^L x^2 \, dx = \frac{L^3}{3}
\]
Thus, the integral becomes:
\[
\int_0^L x \, \lambda(x) \, dx = 2 \times \frac{L^3}{3} = \frac{2L^3}{3}
\]
Finally, the center of mass \( x_{\text{cm}} \) is:
\[
x_{\text{cm}} = \frac{\frac{2L^3}{3}}{L^2} = \frac{2L}{3}
\]
Thus, the center of mass of the rod is at a distance \( \frac{L}{3} \) from the left end.
So the correct answer is (C) \( \frac{L}{3} \).