To solve this problem, we need to work with the properties of a geometric progression (G.P.). Let's denote the first term of the G.P. as \(a\) and the common ratio as \(r\). Therefore, the terms of the sequence can be expressed as follows:
According to the problem, the sum of the second (i.e., \(ar\)) and sixth (i.e., \(ar^5\)) terms is given by:
\(ar + ar^5 = \frac{70}{3}\) ... (1)
The product of the third (i.e., \(ar^2\)) and fifth (i.e., \(ar^4\)) terms is:
\(ar^2 \times ar^4 = 49\)
Which simplifies to:
\(a^2r^6 = 49\) ... (2)
From equation (1), factor out \(ar\):
\(ar(1 + r^4) = \frac{70}{3}\)
Substitute the value of \(ar\) from equation (2):
\(a = \frac{7}{r^3}, \; \text{so} \; ar = \frac{7}{r^2}\)
Plugging it into equation (1):
\(\frac{7}{r^2}(1 + r^4) = \frac{70}{3}\)
Multiplying through by \(r^2\) gives:
\(7(1 + r^4) = \frac{70r^2}{3}\)
Simplifying, this turns into:
\(21 + 21r^4 = 70r^2\)
Or:
\(21r^4 - 70r^2 + 21 = 0\)
Let \(x = r^2\). Then, the equation becomes a quadratic:
\(21x^2 - 70x + 21 = 0\)
Dividing throughout by 7 gives:
\(3x^2 - 10x + 3 = 0\)
Using the quadratic formula, \(x = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\), find the roots:
\(x = \frac{10 \pm \sqrt{(10)^2 - 4 \times 3 \times 3}}{6}\)
\(x = \frac{10 \pm \sqrt{64}}{6}\)
\(x = \frac{10 \pm 8}{6}\)
Thus, \(x = 3\) or \(x = \frac{1}{3}\).
\(r^2 = 3 \; \Rightarrow \; r = \sqrt{3}\) (since \(r\) is positive).
Substitute \(r = \sqrt{3}\) into the expression for \(a\):
\(a = \frac{7}{(\sqrt{3})^3} = \frac{7}{3\sqrt{3}} = \frac{7\sqrt{3}}{9}\)
Thus, calculate the sum of the 4th (\(ar^3\)), 6th (\(ar^5\)), and 8th (\(ar^7\)) terms:
The terms are:
\(ar^3 = \frac{7\sqrt{3}}{9} \cdot 3(\sqrt{3}) = 7\)
\(ar^5 = \frac{7\sqrt{3}}{9} \cdot (\sqrt{3})^5 = 21\)
\(ar^7 = \frac{7\sqrt{3}}{9} \cdot (\sqrt{3})^7 = 63\)
Therefore, the required sum is:
\(7 + 21 + 63 = 91\)
Thus, the sum of the 4th, 6th, and 8th terms is 91.
Given:
\( T_2 + T_6 = \frac{70}{3} \quad \text{and} \quad T_3 \cdot T_5 = 49. \) Let the first term of the geometric progression be \( a \) and the common ratio be \( r \).
The second term is:
\[ T_2 = ar, \] and the sixth term is:
\[ T_6 = ar^5. \]
Given:
\[ ar + ar^5 = \frac{70}{3}. \] Factoring out \( ar \):
\(ar(1 + r^4) = \frac{70}{3}.\) (1)
The third term is:
\[ T_3 = ar^2, \]and the fifth term is:
\[ T_5 = ar^4.\]
Given:
\[ T_3 \times T_5 = ar^2 \times ar^4 = (ar^3)^2 = 49. \]
Taking the square root:
\(ar^3 = 7 \implies a = \frac{7}{r^3}.\) (2)
Substituting the value of \( a \) from equation (2) into equation (1):
\[ \frac{7}{r^3} \times r \times (1 + r^4) = \frac{70}{3}.\]
Simplifying:
\[ \frac{7}{r^2} (1 + r^4) = \frac{70}{3}. \]
Multiplying both sides by \( 3r^2 \):
\[ 21(1 + r^4) = 70r^2. \]
Rearranging terms:
\[ 21 + 21r^4 = 70r^2. \]
Dividing by 7:
\[ 3 + 3r^4 = 10r^2. \]
Letting \( t = r^2 \), we have:
\[ 3 + 3t^2 = 10t. \]
Rearranging:
\[ 3t^2 - 10t + 3 = 0. \]
Solving this quadratic equation using the quadratic formula:
\[ t = \frac{10 \pm \sqrt{100 - 36}}{6} = \frac{10 \pm \sqrt{64}}{6} = \frac{10 \pm 8}{6}.\] This gives:
\[t = \frac{18}{6} = 3 \quad \text{or} \quad t = \frac{2}{6} = \frac{1}{3}.\]
Since the GP is increasing, we take \( t = 3 \),
so:
\[ r^2 = 3 \implies r = \sqrt{3}. \] Using \( r = \sqrt{3} \) in equation (2):
\[ a = \frac{7}{(\sqrt{3})^3} = \frac{7}{3\sqrt{3}} = \frac{7\sqrt{3}}{9}. \] Now, we find the sum of the 4th, 6th, and 8th terms:
\[ T_4 = ar^3, \quad T_6 = ar^5, \quad T_8 = ar^7. \] Calculating:
\[ T_4 + T_6 + T_8 = ar^3 + ar^5 + ar^7 = ar^3 (1 + r^2 + r^4). \] Substituting values:
\[ ar^3 = 7, \quad 1 + r^2 + r^4 = 1 + 3 + 9 = 13. \] Thus:
\[ T_4 + T_6 + T_8 = 7 \times 13 = 91. \] Therefore:
\[ 91. \]
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,