Let's differentiate the right-hand side with respect to $x$: $\frac{d}{dx} \left[ \frac{1}{\alpha} \left(\frac{x}{e}\right)^{\beta x} - \frac{1}{\gamma} \left(\frac{e}{x}\right)^{\delta x} + C \right]$
Let $y = \left(\frac{x}{e}\right)^{\beta x}$. Then $\ln y = \beta x (\ln x - 1)$. $\frac{1}{y} \frac{dy}{dx} = \beta (\ln x - 1) + \beta x \cdot \frac{1}{x} = \beta \ln x$. $\frac{dy}{dx} = \beta \left(\frac{x}{e}\right)^{\beta x} \ln x$.
Let $z = \left(\frac{e}{x}\right)^{\delta x}$. Then $\ln z = \delta x (1 - \ln x)$. $\frac{1}{z} \frac{dz}{dx} = \delta (1 - \ln x) - \delta = -\delta \ln x$. $\frac{dz}{dx} = -\delta \left(\frac{e}{x}\right)^{\delta x} \ln x$.
Therefore, the derivative is: $\frac{\beta}{\alpha} \left(\frac{x}{e}\right)^{\beta x} \ln x + \frac{\delta}{\gamma} \left(\frac{e}{x}\right)^{\delta x} \ln x$
Comparing with the integrand, we have:
$\beta x = 2x \implies \beta = 2$ $\alpha = \beta \implies \alpha = 2$ $\delta x = 2x \implies \delta = 2$ $\gamma = \delta \implies \gamma = 2$ $\alpha + 2\beta + 3\gamma - 4\delta = 2 + 2(2) + 3(2) - 4(2) = 2 + 4 + 6 - 8 = 4$
Answer: 4.
The area enclosed by the closed curve $C$ given by the differential equation $\frac{d y}{d x}+\frac{x+a}{y-2}=0, y(1)=0$ is $4 \pi$.
Let $P$ and $Q$ be the points of intersection of the curve $C$ and the $y$-axis If normals at $P$ and $Q$ on the curve $C$ intersect $x$-axis at points $R$ and $S$ respectively, then the length of the line segment $R S$ is
The statement
\((p⇒q)∨(p⇒r) \)
is NOT equivalent to
Let α, β(α > β) be the roots of the quadratic equation x2 – x – 4 = 0.
If \(P_n=α^n–β^n, n∈N\) then \(\frac{P_{15}P_{16}–P_{14}P_{16}–P_{15}^2+P_{14}P_{15}}{P_{13}P_{14}}\)
is equal to _______.
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 : \(A_2 \rightleftharpoons 2A\)