\(6\sqrt3\)
\(L_1\) : \(\frac{x−3}{2}=\frac{y−2}{3}=\frac{z−1}{−1}\)
\(L_2\) : \(\frac{x+3}{2}=\frac{y-6}{1}=\frac{z−5}{3}\)
Now,
\(\overrightarrow p×\overrightarrow q\) = \(\begin{vmatrix}\hat i& \hat j& \hat k\\ 2 &3 &−1 \\ 2 & 1& 3 \end{vmatrix} =10\hat i−8\hat j−4\hat k\)
\(\overrightarrow a_2−\overrightarrow a_1=6\hat i−4\hat j−4\hat k\)
\(∴S.D=\begin{vmatrix}\frac{60+32+16}{\sqrt{100+64+16}}\end{vmatrix}\)
= \(\frac{108}{\sqrt{180}}=\frac{18}{\sqrt5}\)
MX is a sparingly soluble salt that follows the given solubility equilibrium at 298 K.
MX(s) $\rightleftharpoons M^{+(aq) }+ X^{-}(aq)$; $K_{sp} = 10^{-10}$
If the standard reduction potential for $M^{+}(aq) + e^{-} \rightarrow M(s)$ is $(E^{\circ}_{M^{+}/M}) = 0.79$ V, then the value of the standard reduction potential for the metal/metal insoluble salt electrode $E^{\circ}_{X^{-}/MX(s)/M}$ is ____________ mV. (nearest integer)
[Given : $\frac{2.303 RT}{F} = 0.059$ V]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :

Formula to find distance between two parallel line:
Consider two parallel lines are shown in the following form :
\(y = mx + c_1\) …(i)
\(y = mx + c_2\) ….(ii)
Here, m = slope of line
Then, the formula for shortest distance can be written as given below:
\(d= \frac{|c_2-c_1|}{\sqrt{1+m^2}}\)
If the equations of two parallel lines are demonstrated in the following way :
\(ax + by + d_1 = 0\)
\(ax + by + d_2 = 0\)
then there is a little change in the formula.
\(d= \frac{|d_2-d_1|}{\sqrt{a^2+b^2}}\)