Step 1: Write the differential equation.
\[
\frac{dy}{dx} + \alpha x y = 0
\]
This is a first-order linear ODE.
Step 2: Rearrange.
\[
\frac{dy}{dx} = -\alpha x y
\]
Step 3: Separate variables.
\[
\frac{dy}{y} = -\alpha x dx
\]
Step 4: Integrate.
\[
\int \frac{1}{y} \, dy = -\alpha \int x \, dx
\]
\[
\ln y = -\frac{\alpha x^2}{2} + C
\]
Step 5: Exponential solution.
\[
y = C_1 \, e^{-\frac{\alpha x^2}{2}}
\]
Step 6: Apply initial condition at $x=0, y=1$.
\[
1 = C_1 e^0 \Rightarrow C_1 = 1
\]
So,
\[
y = e^{-\frac{\alpha x^2}{2}}
\]
Step 7: Apply condition at $x=1, y=0.8$.
\[
0.8 = e^{-\frac{\alpha (1)^2}{2}} \Rightarrow \ln(0.8) = -\frac{\alpha}{2}
\]
\[
\alpha = -2 \ln(0.8)
\]
Step 8: Compute numerical value.
\[
\ln(0.8) \approx -0.22314355
\]
\[
\alpha = -2 \times (-0.22314355) = 0.4462871 \approx 0.446
\]
\[
\boxed{0.446}
\]
Let \( u(x, t) \) be the solution of the following initial-boundary value problem: \[ \frac{\partial u}{\partial t} - \frac{\partial^2 u}{\partial x^2} = 0, \quad x \in (0, \pi), \quad t>0, \] with the boundary conditions: \[ u(0, t) = u(\pi, t) = 0, \quad u(x, 0) = \sin 4x \cos 3x. \] Then, for each \( t>0 \), the value of \( u\left( \frac{\pi}{4}, t \right) \) is
Pick the CORRECT solution for the following differential equation:
\[ \frac{dy}{dx} = e^{x - y} \]
The figures, I, II, and III are parts of a sequence. Which one of the following options comes next in the sequence as IV?
For the beam and loading shown in the figure, the second derivative of the deflection curve of the beam at the mid-point of AC is given by \( \frac{\alpha M_0}{8EI} \). The value of \( \alpha \) is ........ (rounded off to the nearest integer).