In your question at the end, you do not specify wheteher your cubic fields are Galois above $Q$, but the whole context of your post suggests that they are. In this case your problem admits a purely Galois theoretic solution (arithmetic will come into play only over $Q$).
Let $p$ be an odd (for simplification) prime and $k$ be a field of characteristic $\neq p $. Denote by $G_k$ the absolute Galois group of $k$. Any cyclic extension of $k$ of degree $p$ (say a $C_p$- extension for short) is the fixed field of a subgroup of index $p$ of $G_k$, and any such subgroup is the kernel of a non trivial homomorphism $G_k \to C_p$, so that the $C_p$-extensions of $k$ are classified by the non trivial elements of the group $Hom(G_k, C_p)$. To progress further, introduce the field $K = k(\mu_p)$, where $\mu_p$ is the group of $p$-th roots of unity, and consider the restriction map $Hom(G_k, C_p) \to Hom(G_K, C_p)$. For any Galois module $X$, $\Delta=Gal(K/k)$ acts on $Hom (G_K , X)$ in the usual way, more precisely via $(\delta, f) \in \Delta \times Hom(G_K, X) \to f^{\delta}$ given by $f^{\delta}(x)= \delta (f(\delta^{-1}(x))$ for $x \in X$ . Note that this action is the only one which is functorial; here $\Delta$ acts trivially on $C_p$. Since $\Delta$ has order prime to $p$, it is classically known that $Hom(G_k, C_p)\cong Hom(G_K, C_p)^{\Delta}$, where the superscript $(.)^{\Delta}$ denotes the invariants under $\Delta$. Since $G_K$ acts trivially on $\mu_p$, one has $Hom(G_K, C_p)\cong Hom(G_K,\mu_p)$ as groups, but not as $\Delta$-modules because of the canonical action of $\Delta$ defined above. Actually, one can check easily that $Hom(G_K, C_p)\cong Hom(G_K,\mu_p)(-1)$, where $(.)(-1)$ denotes the so called "Tate twist", which means that the Galois action on $Hom(G_K,\mu_p)$ has been replaced by a new action defined by $\delta^{new} (f)= \kappa(\delta)^{-1}.\delta^{old}(f)$, where $\kappa$ is the mod $p$ character defined by $\delta(\zeta)=\zeta^{\kappa(\delta)}$ for $\zeta \in \mu_p$ . Consequently, $Hom(G_k, C_p)$ can be identied with the elements $f\in Hom(G_K,\mu_p)$ such that $\delta (f)=\kappa(\delta).f$ (these can be viewed as "eigenvectors" corresponding to the "eigenvalues" $\kappa(\delta)$.)
Now, by Kummer theory, $Hom(G_K,\mu_p)\cong (K^{*}/K^{*})^p$ , which means more concretely that any $C_p$-extension of $K$ is of the form $K(\sqrt [p]a)$, where $a$ represents a class $\bar a \in (K^{*}/K^{*})^p$, and two such extensions $K(\sqrt [p]a)$ and $K(\sqrt [p]b)$ coincide iff $\bar a = \bar b^j$ for a certain $j\neq 0$ mod $p$. Summarizing : two $C_p$-extensions $L$ and $L'$ of $k$ coincide iff the composite fields $L.K = K(\sqrt [p]a)$ and $L'.K = K(\sqrt [p]b)$ coincide, which means that $\delta(\bar a)=\kappa(\delta).\bar a$ and $\bar a = \bar b^j$, $j\neq 0$ mod $p$. This is an "elegant" theoretical way to distinguish between two $C_p$-extensions of $k$, but of course, in concrete examples, it requires some computations - although in your paticular case $k=Q$ and $p=3$, these do not seem especially complicated. For pure cubic fields, i.e. of the form $Q(\sqrt [3] a)$, with $a \in Q^{*}$, they even start in an obvious way ./.