To solve the problem, we need to understand the condition given for the circles touching externally and how the point \((6, 6)\) divides the line segment joining the centers of the circles.
\(\frac{16 + \alpha}{3} = 6 \Rightarrow 16 + \alpha = 18 \Rightarrow \alpha = 2\)
\(\frac{15 + \beta}{3} = 6 \Rightarrow 15 + \beta = 18 \Rightarrow \beta = 3\)
\((8 - 2)^2 = 36\)
\(\left(\frac{15}{2} - 3\right)^2 = {\left(\frac{9}{2}\right)}^2 = \frac{81}{4}\)
So, \(r_1 + r_2 = \frac{15}{2}\).
\(\alpha + \beta = 2 + 3 = 5\)
We know from square of sum, \((r_1 + r_2)^2 = r_1^2 + r_2^2 + 2r_1r_2\).
\(\left(\frac{15}{2}\right)^2 = r_1^2 + r_2^2 + 2r_1r_2\)
\(\frac{225}{4} - 2r_1r_2 = r_1^2 + r_2^2\)
\(r_1^2 + r_2^2 = \frac{225}{4} - 49\)
\(= \frac{225}{4} - \frac{196}{4} = \frac{29}{4}\)
Hence, \((\alpha + \beta) + 4(r_1^2 + r_2^2) = 130\).
The centers of the circles are \((\alpha, \beta)\) for \(C_1\) and \((8, \frac{15}{2})\) for \(C_2\).
Since the point \((6, 6)\) divides the line segment joining the centers in the ratio \(2:1\), apply the section formula:
\[ \frac{16 + \alpha}{3} = 6 \implies 16 + \alpha = 18 \implies \alpha = 2, \]
\[ \frac{15 + \beta}{3} = 6 \implies 15 + \beta = 18 \implies \beta = 3. \]
Thus, the center of \(C_1\) is \((\alpha, \beta) = (2, 3)\).
The circles touch externally at the point \((6, 6)\), so the distance between the centers equals the sum of the radii:
\[ C_1C_2 = r_1 + r_2. \]
Using the distance formula:
\[ C_1C_2 = \sqrt{(2 - 8)^2 + \left(3 - \frac{15}{2}\right)^2}, \]
\[ C_1C_2 = \sqrt{(-6)^2 + \left(-\frac{9}{2}\right)^2} = \sqrt{36 + \frac{81}{4}} = \sqrt{\frac{144}{4} + \frac{81}{4}} = \sqrt{\frac{225}{4}} = \frac{15}{2}. \]
Thus, \(r_1 + r_2 = \frac{15}{2}\).
Now, since the point \((6, 6)\) lies on both circles, for \(C_1\):
\[ (6 - \alpha)^2 + (6 - \beta)^2 = r_1^2, \]
\[ (6 - 2)^2 + (6 - 3)^2 = r_1^2 \implies 4^2 + 3^2 = r_1^2 \implies r_1^2 = 16 + 9 = 25. \]
So, \(r_1 = 5\). Substituting \(r_1 = 5\) into \(r_1 + r_2 = \frac{15}{2}\):
\[ 5 + r_2 = \frac{15}{2} \implies r_2 = \frac{15}{2} - 5 = \frac{5}{2}. \]
Finally, calculate \((\alpha + \beta) + 4(r_1^2 + r_2^2)\):
\[ \alpha + \beta = 2 + 3 = 5, \]
\[ r_1^2 + r_2^2 = 25 + \left(\frac{5}{2}\right)^2 = 25 + \frac{25}{4} = \frac{100}{4} + \frac{25}{4} = \frac{125}{4}, \]
\[ 4(r_1^2 + r_2^2) = 4 \cdot \frac{125}{4} = 125. \]
Thus:
\[ (\alpha + \beta) + 4(r_1^2 + r_2^2) = 5 + 125 = 130. \]
In the figure, triangle ABC is equilateral. 
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 :
