To find the value of \(f(-\log 2)\), we need to solve the given differential equation and use the provided boundary conditions.
The differential equation given is:
\(f'(x) = \alpha f(x) + 3\)
This is a first-order linear differential equation which can be solved using an integrating factor.
The standard form of a first-order linear differential equation is:
\(y' + P(x) y = Q(x)\)
Comparing, we get:
\(P(x) = -\alpha, \quad Q(x) = 3\)
The integrating factor is given by:
\(\mu(x) = e^{\int P(x) \, dx} = e^{-\alpha x}\)
Multiply the entire differential equation by the integrating factor:
\(e^{-\alpha x} f'(x) + \alpha e^{-\alpha x} f(x) = 3 e^{-\alpha x}\)
The left-hand side can be rewritten as the derivative of a product:
\(\frac{d}{dx} \left( e^{-\alpha x} f(x) \right) = 3 e^{-\alpha x}\)
Integrating both sides with respect to \(x\) gives:
\(e^{-\alpha x} f(x) = \int 3 e^{-\alpha x} \, dx = \frac{-3}{\alpha} e^{-\alpha x} + C\)
Therefore, the general solution is:
\(f(x) = \frac{-3}{\alpha} + Ce^{\alpha x}\)
Using the initial condition \(f(0) = 2\):
\(2 = \frac{-3}{\alpha} + C\)
Thus, \(C = 2 + \frac{3}{\alpha}\)
Substitute \(C\) back into the general solution:
\(f(x) = \frac{-3}{\alpha} + \left(2 + \frac{3}{\alpha}\right) e^{\alpha x}\)
Given the condition \(\lim_{x \to \infty} f(x) = 1\), we have:
\(\frac{-3}{\alpha} = 1\), leading to \(\alpha = -3\)
Substitute \(\alpha = -3\) into the solution:
\(f(x) = 1 + \left(2 - 1\right) e^{-3x} = 1 + e^{-3x}\)
Now, calculate \(f(-\log 2)\):
\(f(-\log 2) = 1 + e^{-3(-\log 2)} = 1 + e^{3\log 2}\)
\(e^{3\log 2} = (2^3) = 8\)
Thus, \(f(-\log 2) = 1 + 8 = 9\)
Therefore, the value of \(f(-\log 2)\) is 9.
Given the differential equation:
\[ f'(x) = \alpha f(x) + 3 \]
This is a first-order linear differential equation. We can solve it using an integrating factor (IF).
The integrating factor is given by:
\[ IF = e^{\int \alpha dx} = e^{\alpha x} \]
Multiplying the differential equation by the integrating factor:
\[ e^{\alpha x} f'(x) = \alpha e^{\alpha x} f(x) + 3e^{\alpha x} \]
This simplifies to:
\[ \frac{d}{dx} \left(e^{\alpha x} f(x)\right) = 3e^{\alpha x} \]
Integrating both sides with respect to \( x \):
\[ e^{\alpha x} f(x) = \int 3e^{\alpha x} dx = \frac{3e^{\alpha x}}{\alpha} + C \]
Thus, the general solution is:
\[ f(x) = \frac{3}{\alpha} + Ce^{-\alpha x} \]
Using the initial condition \( f(0) = 2 \):
\[ 2 = \frac{3}{\alpha} + C \] \[ C = 2 - \frac{3}{\alpha} \]
Given that \( \lim_{x \to \infty} f(x) = 1 \):
\[ \lim_{x \to \infty} \left(\frac{3}{\alpha} + \left(2 - \frac{3}{\alpha}\right)e^{-\alpha x}\right) = 1 \]
Since \( e^{-\alpha x} \to 0 \) as \( x \to \infty \), we have:
\[ \frac{3}{\alpha} = 1 \implies \alpha = 3 \]
Substituting \( \alpha = 3 \) back into the solution:
\[ f(x) = 1 + (2 - 1)e^{-3x} = 1 + e^{-3x} \]
Now, we need to find \( f(-\log_2 2) \):
\[ f(-\log_2 2) = 1 + e^{-3(-\log_2 2)} = 1 + e^{3\log_2 2} = 1 + (2^3) = 1 + 8 = 9 \]
Conclusion: \( f(-\log_2 2) = 9 \).
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,