\(^{16}_{7}\text{N} + ^{4}_{2}\text{He} \rightarrow ^{1}_{1}\text{H} + ^{19}_{8}\text{O}\)

4v0 = 1v1 + 19v2 = 20v2 (For max loss of KE)
\(v_0=\frac{v_2}{5}\)
E required \(= (1.008 + 19.003 – 16.006 – 4.003) × 930 = 1.86\)
\(\frac{1}{2}4v_0^2-\frac{1}{2}20v^2=1.86\)
\(\frac{1}{2}4v_0^2-10\frac{v_0^2}{25}20v^2=1.86\)
\(2v_0^2-\frac{2}{5}v_0^2=1.86\)
\(v_0^2=\frac{1.86\times5}{8}\)
KE=\(\frac{1}{2}4v_0^2=2v_0^2=\frac{18.6\times5}{4}\)
\(=2.325\)
To determine the minimum kinetic energy needed by an alpha particle to cause the nuclear reaction:
\[ ^{16}_{7}\text{N} + ^{4}_{2}\text{He} \rightarrow ^{1}_{1}\text{H} + ^{19}_{8}\text{O} \]
we can follow this detailed analysis:
1. Reaction Q-value Calculation
Given the masses:
\( m(^{16}_{7}\text{N}) = 16.006 \, \text{u} \)
\( m(^{4}_{2}\text{He}) = 4.003 \, \text{u} \)
\( m(^{1}_{1}\text{H}) = 1.008 \, \text{u} \)
\( m(^{19}_{8}\text{O}) = 19.003 \, \text{u} \)
\( 1 \, \text{u} = 930 \, \text{MeV}/c^2 \)
The Q-value for the reaction is:
\[Q = (m_{\text{reactants}} - m_{\text{products}}) \times c^2 \]
\[ Q = (16.006 \, \text{u} + 4.003 \, \text{u} - 1.008 \, \text{u} - 19.003 \, \text{u}) \times 930 \, \text{MeV/u} \]
\[ Q = (20.009 \, \text{u} - 20.011 \, \text{u}) \times 930 \, \text{MeV/u}\]
\[ Q = -0.002 \, \text{u} \times 930 \, \text{MeV/u} \]
\[ Q = -1.86 \, \text{MeV} \]
Since \( Q \) is negative, 1.86 MeV of energy must be supplied for the reaction to occur.
2. Kinetic Energy Calculation:
Using momentum conservation for maximum energy loss:
\[ 4v_0 = 1v_1 + 19v_2 = 20v_2 \quad \text{(for max loss of KE)} \]
\[ v_0 = \frac{v_2}{5} \]
The kinetic energy required:
\[ \frac{1}{2}4v_0^2 - \frac{1}{2}20v_2^2 = 1.86 \]
Substituting \( v_0 = \frac{v_2}{5} \):
\[ \frac{1}{2} \left( 4 \left( \frac{v_2}{5} \right)^2 \right) - \frac{1}{2} \left( 20v_2^2 \right) = 1.86 \]
\[\frac{1}{2} \left( 4 \times \frac{v_2^2}{25} \right) - 10v_2^2 = 1.86\]
\[\frac{2v_2^2}{25} - 10v_2^2 = 1.86 \]
\[ 2v_2^2 \left( \frac{1}{25} - \frac{5}{25} \right) = 1.86 \]
\[ 2v_2^2 \left( -\frac{4}{25} \right) = 1.86 \]
\[ v_2^2 = \frac{1.86 \times 25}{-8} \times -1 = \frac{1.86 \times 25}{8} \]
Hence:
\[ v_0^2 = \frac{v_2^2}{25} = \frac{1.86 \times 25}{8 \times 25} = \frac{1.86}{8} \]
The kinetic energy:
\[ \text{KE} = 2v_0^2 = 2 \times \frac{1.86 \times 5}{8} = \frac{1.86 \times 10}{8} = \frac{18.6}{8} = 2.325 \, \text{MeV} \]
Conclusion
Thus, the minimum kinetic energy needed by the alpha particle for the reaction is:
\[ {2.325 \, \text{MeV}} \]
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is:
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Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
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Alpha Decay: In alpha decay, a nucleus emits an alpha particle, consisting of two protons and two neutrons.
Beta Decay: Beta decay involves the emission of a beta particle, which can be a positron or an electron, from an unstable nucleus.
Gamma Decay: Gamma decay releases gamma rays, electromagnetic radiation, to achieve a more stable nuclear state.
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