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: \( f(-\log_2 2) = 9 \).
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

Method used for separation of mixture of products (B and C) obtained in the following reaction is: 