We need to find the Laplace transform, denoted as $Y(s)$, of the solution $y(t)$ to the given second-order linear homogeneous differential equation: $y''(t) + 4y(t) = 0$ with the initial conditions $y(0) = 1$ and $y'(0) = 6$.
The Laplace transform is a powerful tool for solving differential equations. We apply the Laplace transform to both sides of the differential equation. We will use the following standard Laplace transform properties:
Applying these properties to the equation $y''(t) + 4y(t) = 0$, we get:
$L\{y''(t)\} + 4L\{y(t)\} = L\{0\}$
Substituting the properties:
$(s^2 Y(s) - s y(0) - y'(0)) + 4Y(s) = 0$
Now, we substitute the given initial conditions, $y(0) = 1$ and $y'(0) = 6$, into the transformed equation:
$(s^2 Y(s) - s(1) - 6) + 4Y(s) = 0$
This simplifies to:
$s^2 Y(s) - s - 6 + 4Y(s) = 0$
Our goal is to find the expression for $Y(s)$. We can rearrange the equation to isolate $Y(s)$. First, group the terms containing $Y(s)$:
$(s^2 + 4)Y(s) - s - 6 = 0$
Next, move the constant and $s$ terms to the right side of the equation:
$(s^2 + 4)Y(s) = s + 6$
Finally, divide by $(s^2 + 4)$ to solve for $Y(s)$:
$Y(s) = \frac{s + 6}{s^2 + 4}$
To match the format of the options provided, we can split the fraction:
$Y(s) = \frac{s}{s^2 + 4} + \frac{6}{s^2 + 4}$
The Laplace transformation $Y(s)$ of the solution $y(t)$ for the given differential equation and initial conditions is:
$Y(s) = \frac{s}{s^2 + 4} + \frac{6}{s^2 + 4}$
This result corresponds to option 3.
| List-I | List-II |
| Electronic Configuration | First Ionisation energy (kJ mol$^{-1}$) |
| (A). ns$^2$ | (I). 2100 |
| (B). ns$^2$np$^1$ | (II). 1400 |
| (C). ns$^2$np$^3$ | (III). 800 |
| (D). ns$^2$np$^6$ | (IV). 900 |
| List-I | List-II |
| Spectroscopy | Property |
| (A). Raman | (I). Polarizability |
| (B). FTIR | (II). Dipole Moment |
| (C). UV-Visible | (III). Absorbance |
| (D). NMR | (IV). Spin |