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:
\[ (\alpha + \beta) + 4(r_1^2 + r_2^2) = 5 + 125 = 130. \]
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,