To solve the problem, we need to evaluate the given integral condition: \(\int_0^x t f(t) \, dt = x^2 f(x)\) for \(x > 0\) and find \( f(6) \). First, differentiate both sides of the equation with respect to \(x\). The left side is an integral of the form \(\int_0^x u f(u) \, du\), which can be differentiated using the Leibniz rule for differentiation under the integral sign:
\(\frac{d}{dx}\left(\int_0^x tf(t) \, dt\right) = x f(x) + \int_0^x t \frac{d}{dx}f(t) \, dt\).
The right side of the equation differentiated with respect to \(x\) gives:
\(\frac{d}{dx}(x^2 f(x)) = 2x f(x) + x^2 f'(x)\).
Equating the derivatives of both sides:
\(x f(x) + \int_0^x t f'(t) \, dt = 2x f(x) + x^2 f'(x).\)
By comparing both sides, \(\int_0^x t f'(t) \, dt\) needs to satisfy \(x f(x) = 2x f(x) + x^2 f'(x)\).
This simplifies to:
\(0 = x f(x) + x^2 f'(x)\).
Rearranging terms gives us:
\(x f(x)(1 + x f'(x)/f(x)) = 0\).
Since \(x > 0\), it implies:
\(f(x) + x f'(x) = 0\), such that \(f(x)\) satisfies the differential equation \(f'(x)/f(x) = -1/x\).
This differential equation can be solved by separating variables:
\(\frac{d}{dx}\ln|f(x)| = -\frac{1}{x}\).
Integrate both sides:
\(\ln|f(x)| = -\ln|x| + C\) where \(C\) is the constant of integration.
\(|f(x)| = \frac{e^C}{x}\) gives our function \(f(x) = \frac{k}{x}\) where \(k = e^C\) is a constant.
Since \( f(2) = 3 \), substitute into the function:
\(f(2) = \frac{k}{2} = 3\) which implies \(k = 6\).
Therefore, the function is \(f(x) = \frac{6}{x}\).
Finally, we compute \( f(6) \): \(f(6) = \frac{6}{6} = 1\).
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).
Let \( T_r \) be the \( r^{\text{th}} \) term of an A.P. If for some \( m \), \( T_m = \dfrac{1}{25} \), \( T_{25} = \dfrac{1}{20} \), and \( \displaystyle\sum_{r=1}^{25} T_r = 13 \), then \( 5m \displaystyle\sum_{r=m}^{2m} T_r \) is equal to: