In Nielsen and Chuang we define the partial trace operator, defined as
$$\operatorname{tr}_2(|a_1\rangle\langle a_2| \otimes |b_1\rangle\langle b_2|) = |a_1\rangle\langle a_2| \operatorname{tr}(|b_1\rangle\langle b_2|)$$
They go on to say that $\operatorname{tr}_2(|11\rangle\langle00|) = |1\rangle\langle0|\langle0|1\rangle$, which presumably means that $|11\rangle\langle00| = |1\rangle\langle0|\otimes|1\rangle\langle0|$, but how did we arrive at this? Can a similar expression be derived for multi-qubit states?