Step 1: Applying the Law of Conservation of Momentum
Since the body is initially at rest, the total momentum before the explosion is zero. The total momentum after the explosion must also be zero to satisfy the law of conservation of momentum.
The masses of the pieces are in the ratio \(1:1:2\), so we can denote the masses of the pieces as \(m_1 = m\), \(m_2 = m\), and \(m_3 = 2m\).
\( \text{Total momentum before explosion} = 0 \)
\( \text{Total momentum after explosion} = \text{momentum of piece 1} + \text{momentum of piece 2} + \text{momentum of piece 3} = 0 \)
\[m_1 v_1 + m_2 v_2 + m_3 v_3 = 0\] Where:
- \(v_1 = 30 \, \text{m/s}\) (velocity of first piece)
- \(v_2 = 40 \, \text{m/s}\) (velocity of second piece)
- \(v_3\) is the velocity of the third piece.
Step 2: Resolving Momentum Components Since the pieces fly off perpendicular to each other, we can resolve the momentum into two components: horizontal and vertical.
In the horizontal direction: \[ m \cdot 30 + m \cdot 0 + 2m \cdot v_{3x} = 0 \quad \Rightarrow \quad 30 + 2v_{3x} = 0 \quad \Rightarrow \quad v_{3x} = -15 \, \text{m/s} \]
In the vertical direction: \[ m \cdot 0 + m \cdot 40 + 2m \cdot v_{3y} = 0 \quad \Rightarrow \quad 40 + 2v_{3y} = 0 \quad \Rightarrow \quad v_{3y} = -20 \, \text{m/s} \]
Step 3: Calculating the Velocity of the Third Piece The total velocity of the third piece is the vector sum of the horizontal and vertical components of velocity: \[ v_3 = \sqrt{v_{3x}^2 + v_{3y}^2} = \sqrt{(-15)^2 + (-20)^2} = \sqrt{225 + 400} = \sqrt{625} = 25 \, \text{m/s} \] Final Answer: The velocity of the third piece is \(25 \, \text{m/s}\).
A two-level quantum system has energy eigenvalues
\( E_1 \) and \( E_2 \). A perturbing potential
\( H' = \lambda \Delta \sigma_x \) is introduced, where
\( \Delta \) is a constant having dimensions of energy,
\( \lambda \) is a small dimensionless parameter, and
\( \sigma_x = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix} \).
The magnitudes of the first and the second order corrections to
\( E_1 \) due to \( H' \), respectively, are:
Consider a two-level system with energy states \( +\epsilon \) and \( -\epsilon \). The number of particles at \( +\epsilon \) level is \( N+ \) and the number of particles at \( -\epsilon \) level is \( N- \). The total energy of the system is \( E \) and the total number of particles is \( N = N+ + N- \). In the thermodynamic limit, the inverse of the absolute temperature of the system is:
(Given: \( \ln N! \approx N \ln N - N \))