Matrix Singularity Resonance
1. **Problem 1:** Given matrix $$A = \begin{pmatrix} x - 1 & j \\ j2y - jx & j \end{pmatrix}$$ where $$j = \sqrt{-1}$$, find real values of $$x$$ and $$y$$ such that $$A$$ is singular.
2. **Recall:** A matrix is singular if its determinant is zero.
3. **Calculate determinant:**
$$\det(A) = (x - 1) \cdot j - j \cdot (j2y - jx)$$
4. Simplify the second term:
$$j \cdot (j2y - jx) = j^2 2y - j^2 x = (-1) 2y - (-1) x = -2y + x$$
5. Substitute back:
$$\det(A) = j(x - 1) - (-2y + x) = j(x - 1) + 2y - x$$
6. For $$\det(A) = 0$$, real and imaginary parts must be zero separately:
- Real part: $$2y - x = 0$$
- Imaginary part: $$x - 1 = 0$$
7. Solve:
- From imaginary part: $$x = 1$$
- Substitute into real part: $$2y - 1 = 0 \Rightarrow y = \frac{1}{2}$$
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8. **Problem 2:** Given impedance formula for parallel circuit:
$$\frac{1}{Z} = \frac{1}{R + j\omega L + \frac{1}{j\omega C}}$$
with $$R=1$$, $$L=2$$, $$C=0.5$$, find $$\omega > 0$$ for resonance (when $$Z$$ is real).
9. **Rewrite denominator:**
$$R + j\omega L + \frac{1}{j\omega C} = R + j\omega L - \frac{j}{\omega C} = R + j\left(\omega L - \frac{1}{\omega C}\right)$$
10. For $$Z$$ to be real, denominator must be purely real or imaginary part zero:
$$\omega L - \frac{1}{\omega C} = 0$$
11. Solve for $$\omega$$:
$$\omega L = \frac{1}{\omega C} \Rightarrow \omega^2 = \frac{1}{LC}$$
12. Substitute values:
$$\omega^2 = \frac{1}{2 \times 0.5} = \frac{1}{1} = 1$$
13. Therefore:
$$\omega = 1$$ (since $$\omega > 0$$)
**Final answers:**
- For singular matrix: $$x = 1$$, $$y = \frac{1}{2}$$
- For resonance frequency: $$\omega = 1$$