Concept:
If
\[
\vec{r}\times\vec{a}=\vec{c}\times\vec{a},
\]
then
\[
(\vec{r}-\vec{c})\times\vec{a}=0.
\]
This means the vector \( \vec{r}-\vec{c} \) is parallel to \( \vec{a} \). Hence, the line can be written in vector form as
\[
\vec{r}=\vec{c}+\lambda\vec{a}.
\]
Step 1: Writing the first line in parametric form.
Given,
\[
\vec{r}\times\vec{a}=\vec{b}\times\vec{a}.
\]
Therefore,
\[
(\vec{r}-\vec{b})\times\vec{a}=0.
\]
Hence,
\[
\vec{r}-\vec{b}=\lambda\vec{a}.
\]
Now,
\[
\vec{a}=\hat{i}+\hat{j}=(1,1,0),
\]
and
\[
\vec{b}=\hat{i}-\hat{k}=(1,0,-1).
\]
Thus,
\[
\vec{r}=(1,0,-1)+\lambda(1,1,0).
\]
So,
\[
\vec{r}=(1+\lambda,\lambda,-1).
\]
Therefore, the first line is
\[
L_1:(1+\lambda,\lambda,-1).
\]
Step 2: Writing the second line in parametric form.
Given,
\[
\vec{r}\times\vec{b}=\vec{a}\times\vec{b}.
\]
Therefore,
\[
(\vec{r}-\vec{a})\times\vec{b}=0.
\]
Hence,
\[
\vec{r}-\vec{a}=\mu\vec{b}.
\]
Substituting the values,
\[
\vec{r}=(1,1,0)+\mu(1,0,-1).
\]
Thus,
\[
\vec{r}=(1+\mu,1,-\mu).
\]
Therefore, the second line is
\[
L_2:(1+\mu,1,-\mu).
\]
Step 3: Equating corresponding coordinates.
At the point of intersection,
\[
(1+\lambda,\lambda,-1)=(1+\mu,1,-\mu).
\]
Comparing the \( y \)-coordinates:
\[
\lambda=1.
\]
Comparing the \( z \)-coordinates:
\[
-1=-\mu
\]
\[
\mu=1.
\]
Comparing the \( x \)-coordinates:
\[
1+\lambda=1+\mu
\]
\[
1+1=1+1.
\]
Hence, the equations are consistent.
Step 4: Finding the point of intersection.
Substituting
\[
\lambda=1
\]
into
\[
(1+\lambda,\lambda,-1),
\]
we get
\[
(1+1,1,-1).
\]
Therefore,
\[
\boxed{(2,1,-1)}.
\]