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Question: How do you find a vector orthogonal to both \(i+j\) and \(i+k\)?...

How do you find a vector orthogonal to both i+ji+j and i+ki+k?

Explanation

Solution

We can let the unit vector orthogonal to both i+ji+j and i+ki+k as r=ai+bj+ckr=ai+bj+ck. Unit vector means its magnitude must be one, which will give a2+b2+c2=1{{a}^{2}}+{{b}^{2}}+{{c}^{2}}=1. Also, since the vector rr is orthogonal to both i+ji+j and i+ki+k, its dot product with both of these vectors will be equal to zero. On putting these dot product equal to zero, we will get two equations in terms of aa, bb and cc which on solving with a2+b2+c2=1{{a}^{2}}+{{b}^{2}}+{{c}^{2}}=1 will solve for the unit vector rr.

Complete step by step solution:
Let us consider the two vectors given in the above question as uu and vv so that we can write the vector equations
u=i+j.......(i)\Rightarrow u=i+j.......\left( i \right)
And
v=i+k.......(ii)\Rightarrow v=i+k.......\left( ii \right)
Now, let the unit vector orthogonal to both of the vectors uu and vv be rr such that
r=(ai+bj+ck)........(iii)\Rightarrow r=\left( ai+bj+ck \right)........\left( iii \right)
Now, since rr is a unit vector, we can write
r=1\Rightarrow \left| r \right|=1
From (iii) we can write
a2+b2+c2=1\Rightarrow \sqrt{{{a}^{2}}+{{b}^{2}}+{{c}^{2}}}=1
On squaring both the sides, we get
a2+b2+c2=1.......(iv)\Rightarrow {{a}^{2}}+{{b}^{2}}+{{c}^{2}}=1.......\left( iv \right)
Now, since rr is orthogonal to uu, we can write
ru=0\Rightarrow r\cdot u=0
Putting (i) and (iii) in the above equation, we get

& \Rightarrow \left( ai+bj+ck \right)\cdot \left( i+j \right)=0 \\\ & \Rightarrow a\left( 1 \right)+b\left( 1 \right)+c\left( 0 \right)=0 \\\ & \Rightarrow a+b=0.......\left( v \right) \\\ \end{aligned}$$ Also, since $r$ is orthogonal to $v$, we can write $\Rightarrow r\cdot v=0$ Putting (ii) and (iii) in the above equation, we get $$\begin{aligned} & \Rightarrow \left( ai+bj+ck \right)\cdot \left( i+k \right)=0 \\\ & \Rightarrow a\left( 1 \right)+b\left( 0 \right)+c\left( 1 \right)=0 \\\ & \Rightarrow a+c=0.......\left( vi \right) \\\ \end{aligned}$$ Subtracting (vi) from (v) we get $\begin{aligned} & \Rightarrow a+b-\left( a+c \right)=0 \\\ & \Rightarrow a+b-a-c=0 \\\ & \Rightarrow b-c=0 \\\ & \Rightarrow b=c........\left( vii \right) \\\ \end{aligned}$ Also, subtracting $b$ from both sides of the equation (v), we get $\begin{aligned} & \Rightarrow a+b-b=0-b \\\ & \Rightarrow a=-b.......\left( viii \right) \\\ \end{aligned}$ From (vii) and (viii) we can write $\begin{aligned} & \Rightarrow -a=b=c=\lambda \left( say \right) \\\ & \Rightarrow a=-\lambda ,b=\lambda ,c=\lambda .......\left( ix \right) \\\ \end{aligned}$ Therefore, the vector $r$ becomes $\begin{aligned} & \Rightarrow r=-\lambda i+\lambda j+\lambda k \\\ & \Rightarrow r=\lambda \left( -i+j+k \right).......\left( x \right) \\\ \end{aligned}$ Putting (ix) in (iv) we get $$\begin{aligned} & \Rightarrow {{\left( -\lambda \right)}^{2}}+{{\lambda }^{2}}+{{\lambda }^{2}}=1 \\\ & \Rightarrow {{\lambda }^{2}}+{{\lambda }^{2}}+{{\lambda }^{2}}=1 \\\ & \Rightarrow 3{{\lambda }^{2}}=1 \\\ & \Rightarrow {{\lambda }^{2}}=\dfrac{1}{3} \\\ \end{aligned}$$ On solving the above equation, we get $$\begin{aligned} & \Rightarrow \lambda =\pm \dfrac{1}{\sqrt{3}} \\\ & \Rightarrow \lambda =\dfrac{1}{\sqrt{3}},\lambda =-\dfrac{1}{\sqrt{3}} \\\ \end{aligned}$$ Putting $\lambda =\dfrac{1}{\sqrt{3}}$ in (x) we get $\Rightarrow r=\dfrac{1}{\sqrt{3}}\left( -i+j+k \right)$ Similarly, putting $\lambda =-\dfrac{1}{\sqrt{3}}$ we get $\Rightarrow r=-\dfrac{1}{\sqrt{3}}\left( -i+j+k \right)$ **Hence, the unit vectors perpendicular to the given vectors are $\dfrac{1}{\sqrt{3}}\left( -i+j+k \right)$ and $-\dfrac{1}{\sqrt{3}}\left( -i+j+k \right)$.** **Note:** We can also use the concept of cross product to obtain the unit vector perpendicular to $u$ and $v$. Since the unit vector $r$ is orthogonal to both $u$ and $v$, it must be normal to the plane formed by $u$ and $v$, which means that it must be parallel to the cross product $u\times v$. So the unit vector $r$ can be written as $r=\pm \dfrac{u\times v}{\left| u\times v \right|}$.