Tensor multiplication is just a generalization of matrix multiplication which is just a generalization of vector multiplication.
Matrix multiplication is defined as:
$$ A_i \cdot B_j = C_{i, j}$$
where $i$ is the $i^{th}$ row, $j$ is the $j^{th}$ column, and $\cdot$ is the dot product. Therefore it just a series of dot products.
One can then see how this extends to tensors:
$$\mathbf{A}_{i} \cdot \mathbf{B}_{j} = \mathbf{C}_{i, j} $$
where $i$ is the $i^{th}$ row-wise matrix of the tensor, and $j$ is the $j^{th}$ column-wise matrix of the tensor... and is therefore just a series of matrix multiplications - or a series of a series of dot products.
Assuming all tensors are of rank three(it can be described with three coordinates):
$$\mathbf{A} \otimes \mathbf{B} = \mathbf{A}_{i, j} \cdot \mathbf{B}_{j, k} = \mathbf{C}_{i, j, k}$$
which means the $(i,j)^{th}$ vector of $\mathbf{A}$ times the $(j, k)^{th}$ vector of $\mathbf{B}$.