The problem provides a system of three linear equations in variables \(x, y, z\) with two parameters, \(\lambda\) and \(\mu\). We are told that the system has infinitely many solutions, and we need to find the value of \((\lambda - \mu)\).
For a system of linear equations of the form \(AX = B\), where \(A\) is the coefficient matrix and \(B\) is the constant vector, the condition for having infinitely many solutions is that the determinant of the coefficient matrix is zero, and the determinants of the matrices formed by replacing a column of \(A\) with \(B\) are also zero. In terms of Cramer's rule notation, this means:
\[ \Delta = \det(A) = 0 \]and
\[ \Delta_x = \Delta_y = \Delta_z = 0 \]where \(\Delta_x, \Delta_y, \Delta_z\) are the determinants of the matrices obtained by replacing the x, y, and z columns of \(A\) with the constant vector, respectively.
Step 1: Write down the determinants \(\Delta\) and \(\Delta_y\).
The given system of equations is:
\[ 2x + 7y + \lambda z = 3 \] \[ 3x + 2y + 5z = 4 \] \[ x + \mu y + 32z = -1 \]The determinant of the coefficient matrix is:
\[ \Delta = \begin{vmatrix} 2 & 7 & \lambda \\ 3 & 2 & 5 \\ 1 & \mu & 32 \end{vmatrix} \]The determinant \(\Delta_y\) is obtained by replacing the second column (coefficients of y) with the constant terms:
\[ \Delta_y = \begin{vmatrix} 2 & 3 & \lambda \\ 3 & 4 & 5 \\ 1 & -1 & 32 \end{vmatrix} \]Since \(\Delta_y\) does not contain the parameter \(\mu\), it is advantageous to evaluate it first to find \(\lambda\).
Step 2: Set \(\Delta_y = 0\) and solve for \(\lambda\).
For the system to have infinitely many solutions, we must have \(\Delta_y = 0\).
\[ \begin{vmatrix} 2 & 3 & \lambda \\ 3 & 4 & 5 \\ 1 & -1 & 32 \end{vmatrix} = 0 \]Expanding along the first row:
\[ 2(4 \cdot 32 - 5 \cdot (-1)) - 3(3 \cdot 32 - 5 \cdot 1) + \lambda(3 \cdot (-1) - 4 \cdot 1) = 0 \] \[ 2(128 + 5) - 3(96 - 5) + \lambda(-3 - 4) = 0 \] \[ 2(133) - 3(91) - 7\lambda = 0 \] \[ 266 - 273 - 7\lambda = 0 \] \[ -7 - 7\lambda = 0 \] \[ 7\lambda = -7 \implies \lambda = -1 \]Step 3: Set \(\Delta = 0\) and substitute the value of \(\lambda\) to solve for \(\mu\).
For infinitely many solutions, we must also have \(\Delta = 0\).
\[ \Delta = \begin{vmatrix} 2 & 7 & \lambda \\ 3 & 2 & 5 \\ 1 & \mu & 32 \end{vmatrix} = 0 \]Expanding along the first row:
\[ 2(2 \cdot 32 - 5 \cdot \mu) - 7(3 \cdot 32 - 5 \cdot 1) + \lambda(3 \cdot \mu - 2 \cdot 1) = 0 \] \[ 2(64 - 5\mu) - 7(96 - 5) + \lambda(3\mu - 2) = 0 \] \[ 128 - 10\mu - 7(91) + \lambda(3\mu - 2) = 0 \] \[ 128 - 10\mu - 637 + \lambda(3\mu - 2) = 0 \] \[ -509 - 10\mu + \lambda(3\mu - 2) = 0 \]Now, substitute the value \(\lambda = -1\) into this equation:
\[ -509 - 10\mu + (-1)(3\mu - 2) = 0 \] \[ -509 - 10\mu - 3\mu + 2 = 0 \] \[ -507 - 13\mu = 0 \] \[ 13\mu = -507 \] \[ \mu = -\frac{507}{13} = -39 \]Step 4: Calculate the value of \((\lambda - \mu)\).
We have found \(\lambda = -1\) and \(\mu = -39\).
\[ \lambda - \mu = (-1) - (-39) = -1 + 39 = 38 \]The value of \((\lambda - \mu)\) is 38.
For the system to have infinitely many solutions, the determinant of the coefficient matrix must be zero. We set:
\[D = D_1 = D_2 = D_3 = 0\]
Calculating \( D_3 \):
\[D_3 = \begin{vmatrix}2 & 7 & 3 \\3 & 2 & 4 \\1 & \mu & -1\end{vmatrix}= 0\]
Expanding, we get:
\[2 \begin{vmatrix}2 & 4 \\\mu & -1\end{vmatrix}- 7 \begin{vmatrix}3 & 4 \\1 & -1\end{vmatrix}+ 3 \begin{vmatrix}3 & 2 \\1 & \mu\end{vmatrix}= 0\]
Solving for \( \mu \), we find:
\[\mu = -39\]
Now, calculating \( D \) with \( \lambda \) in place:
\[D = \begin{vmatrix}2 & 7 & \lambda \\3 & 2 & 5 \\1 & -39 & 32\end{vmatrix}= 0\]
Solving this determinant, we get:
\[\lambda = -1\]
Thus, \( \lambda - \mu = -1 - (-39) = 38 \).
The heat generated in 1 minute between points A and B in the given circuit, when a battery of 9 V with internal resistance of 1 \(\Omega\) is connected across these points is ______ J. 
The given circuit works as: 
Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}