Well, you should see that if $V$ and $W$ are arbitrary finite-dimensional vector spaces over the same field, and $A:V\rightarrow W$ is a linear isomorphism (invertible linear transformation) then the image of a linearly independent set of vectors will remain independent under the action of $A$.
For example, let $E=\{e_1,...,e_k\}\subset V$ be a set of linearly independent vectors in $V$,and let $Ae_1,...Ae_k$ be their images in $W$.
Assume, that the images $Ae_1,...,Ae_k$ are dependent. Then there exist a linear combination of them with at least some nonzero coefficients, $$ \alpha_1Ae_1+...\alpha_kAe_k, $$ that is the $0_W$ zero vector in $W$. Now, using linearity, $$ 0_W=\alpha_1Ae_1+...\alpha_kAe_k=A(\alpha_1e_1+...+\alpha_ke_k), $$ meaning, that $\alpha_1e_1+...+\alpha_ke_k\in \ker A$. But, since $A$ is invertible, its kernel must be trivial, so $\alpha_1e_1+...+\alpha_ke_k=0_V$. But some of the $\alpha_i$ coefficients are nonzero, which implies that $E$ is linearly dependent, which is a contradiction.
Actually, this doesn't require $A$ to be invertible, just that its kernel is trivial.
You can check easily that the map that maps your vectors in $V$ to their components in $\mathbb{R}^n$ is a linear isomorphism, therefore, by what we derived now, it preserves linear independence.