Let's solve the given problem step-by-step.
Given that \(AA^T = I\), matrix \(A\) is orthogonal.
We need to find the value of:
\(\frac{1}{2}A[(A+A^T)^2+(A-A^T)^2]\)
First, we expand the expression \((A+A^T)^2\):
\((A + A^T)^2 = A^2 + AA^T + A^TA + (A^T)^2\)
Since \((AA^T = I)\) and \((A^TA = I)\), we have:
Similarly, expand the expression \((A-A^T)^2\):
\((A - A^T)^2 = A^2 - AA^T - A^TA + (A^T)^2\)
Adding both expansions, we get:
\((A + A^T)^2 + (A - A^T)^2 = (A^2 + I + I + (A^T)^2) + (A^2 - I - I + (A^T)^2)\)
The terms \(-I\) and \(+I\) cancel each other, so:
\(= 2A^2 + 2(A^T)^2\)
Substituting back into the original expression:
\(\frac{1}{2}A[2(A^2 + (A^T)^2)] = A(A^2 + (A^T)^2)\)
Now simplify:
Since \((A^T)^2 = A^2\) for orthogonal matrices:
\(= A(A^2 + A^2)\)
\(= A(2A^2)\)
\(= 2A^3\)
The given problem aims to simplify to reveal a simpler form, so we double-check another route:
\(= A^3 + A^T\) (since \((A^T)^2 = A^2\)) aligns to the option
Thus, the correct answer is:
A3+AT
Given that \(AA^\top = I\), we can substitute this property in the expression.
\[ \frac{1}{2} A \left[(A + A^\top)^2 + (A - A^\top)^2\right] \]
Expanding \((A + A^\top)^2\) and \((A - A^\top)^2\), we get:
\[ \frac{1}{2} A \left[A^2 + (A^\top)^2 + 2AA^\top + A^2 + (A^\top)^2 - 2AA^\top\right] \]
\[ = A \left[A^2 + (A^\top)^2\right] \]
\[ = A^3 + A^\top \]
So, the correct answer is: \(A^3 + A^\top\)
Two positively charged particles \(m_1\) and \(m_2\) have been accelerated across the same potential difference of 200 keV. Given mass of \(m_1 = 1 \,\text{amu}\) and \(m_2 = 4 \,\text{amu}\). The de Broglie wavelength of \(m_1\) will be \(x\) times that of \(m_2\). The value of \(x\) is _______ (nearest integer). 