I thought of this method:
Suppose the given equations are:
$$a_1x+a_2y+a_3z=d_1$$ $$b_1x+b_2y+b_3z=d_2$$ $$c_1x+c_2y+c_3z=d_3$$
Let $\vec{p}=x\hat{i}+y\hat{j}+z\hat{k},\:\:\:\: \vec{a}=a_1\hat{i}+a_2\hat{j}+a_3\hat{k},\:\:\:\: \vec{b}=b_1\hat{i}+b_2\hat{j}+b_3\hat{k},\:\:\:\: \vec{c}=c_1\hat{i}+c_2\hat{j}+c_3\hat{k}$
Then, $d_1=\vec{p}\cdot \vec{a},\:\:\:\: d_2=\vec{p}\cdot \vec{b},\:\:\:\: d_3=\vec{p}\cdot \vec{c}$
Now, evaluate $\vec{1}=\vec{a}, \:\:\:\:\vec{2}=\vec{b}-\frac{(\vec{a}\cdot\vec{b})\vec{a}}{|\vec{a}|^2},\:\:\:\: \vec{3}=\vec{c}-\frac{(\vec{c}\cdot\vec{a})\vec{a}}{|\vec{a}|^2}-\frac{(\vec{c}\cdot \vec{b})\vec{b}}{|\vec{b}|^2}$. The vectors $\frac{\vec{1}}{|\vec{1}|}, \frac{\vec{2}}{|\vec{2}|}, \frac{\vec{3}}{|\vec{3}|}$ are perpendicular to each other. The components of $\vec{p}$ along these three vectors are $\frac{d_1}{|\vec{a}||\vec{1}|}$, $\frac{1}{|\vec{2}|}(d_2-\frac{(\vec{a}\cdot\vec{b})d_1}{|\vec{a}|^2})$, and $\frac{1}{|\vec{3}|}(d_3-\frac{(\vec{c}\cdot\vec{a})d_1}{|\vec{a}|^2}-\frac{(\vec{c}\cdot \vec{b})d_2}{|\vec{b}|^2})$ respectively.
Therefore, $$\vec{p}=d_1\frac{\vec{1}}{|\vec{1}|^2}+\left(d_2-\frac{(\vec{a}\cdot\vec{b})d_1}{|\vec{a}|^2}\right)\frac{\vec{2}}{|\vec{2}|^2}+\left(d_3-\frac{(\vec{c}\cdot\vec{a})d_1}{|\vec{a}|^2}-\frac{(\vec{c}\cdot \vec{b})d_2}{|\vec{b}|^2}\right)\frac{\vec{3}}{|\vec{3}|^2}$$
Is this method more or less expensive than Cramer's Rule? Or Does it involve the same calculations as in Cramer's rule?