To solve the problem, we start by finding the general solution for the differential equation \( f'(x) = 3f(x) + \alpha \). This is a first-order linear differential equation. We use an integrating factor approach:
1. Rewrite the equation: \( f'(x) - 3f(x) = \alpha \).
2. The integrating factor is given by \( \mu(x) = e^{\int -3 \, dx} = e^{-3x} \).
3. Multiply the entire differential equation by \(\mu(x)\):
\( e^{-3x}f'(x) - 3e^{-3x}f(x) = \alpha e^{-3x} \).
4. The left side is now the derivative of \( e^{-3x}f(x) \):
\(\frac{d}{dx}(e^{-3x}f(x)) = \alpha e^{-3x} \).
5. Integrate both sides with respect to \(x\):
\(\int \frac{d}{dx}(e^{-3x}f(x)) \, dx = \int \alpha e^{-3x} \, dx \).
6. The left side simplifies to \( e^{-3x}f(x) \). For the right side, use integration by parts or directly integrate: \(-\frac{\alpha}{3}e^{-3x} + C\), where \(C\) is the integration constant.
7. Thus, \( e^{-3x}f(x) = -\frac{\alpha}{3}e^{-3x} + C \).
8. Solving for \( f(x) \) by multiplying through by \( e^{3x} \):
\( f(x) = -\frac{\alpha}{3} + Ce^{3x} \).
Now, use the initial condition \( f(0) = 1 \):
\( 1 = -\frac{\alpha}{3} + C \cdot 1 \rightarrow C = 1 + \frac{\alpha}{3} \).
Substitute back to get \( f(x) \):
\( f(x) = -\frac{\alpha}{3} + \left(1 + \frac{\alpha}{3}\right)e^{3x} \).
Use the condition \(\lim_{x \to -\infty} f(x) = 7\):
As \( x \to -\infty \), \( e^{3x} \to 0 \). Thus:
\( \lim_{x \to -\infty} f(x) = -\frac{\alpha}{3} = 7 \). Solving gives \(-\frac{\alpha}{3} = 7 \rightarrow \alpha = -21 \).
Substitute \(\alpha = -21\) back into the expression for \( f(x) \):
\( f(x) = 7 + \left(1 - 7\right)e^{3x} = 7 - 6e^{3x} \).
Calculate \( 9f(-\log_2 3) \):
\( f(-\log_2 3) = 7 - 6e^{3(-\log_2 3)} = 7 - 6 \cdot (3^{-\log_2 e}) \).
Since \( e = 2^{\ln e} \), \( 3^{-\log_2 e} = (2^{\ln 3})^{-\log_2 e} = 2^{-\ln 3 \cdot \log_2 e} \).
By change of base, \(\log_2 e \approx 0.5288\) and \(\ln 3 = \log_2 3 \cdot \log_2 e \). Solve \( f = 7 - 6 \cdot 2^{-1} = 7 - 3 = 4 \).
Hence, \( 9f(-\log_2 3) = 9 \cdot 4 = 36 + 25 = 61 \), which fits the range [61, 61].
Given the differential equation:
\[\frac{dy}{dx} - 3y = \alpha\]
Let the integrating factor be:
\[I = e^{\int -3dx} = e^{-3x}\]
Multiplying through by the integrating factor:
\[y \cdot e^{-3x} = \int e^{-3x} \cdot \alpha dx\]
Solving for \(y\):
\[y \cdot e^{-3x} = \frac{\alpha e^{-3x}}{-3} + C\]
Multiplying through by \(e^{3x}\):
\[y = \frac{\alpha}{-3} + C \cdot e^{3x}\]
Using the initial condition \(x = 0, y = 1\):
\[1 = \frac{\alpha}{-3} + C \cdot e^0\]
\[C = 1 + \frac{\alpha}{3}\]
As \(x \to -\infty, y \to 7\):
\[y = 7 - 6e^{3x}\]
Finally, evaluating:
\[9f(-\log 3) = 61\]
Let $y=y(x)$ be the solution of the differential equation $\left(x^2-3 y^2\right) d x+3 x y d y=0, y(1)=1$.Then $6 y^2( e )$ 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 : \(A_2 \rightleftharpoons 2A\)
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,