In a nuclear reaction of `alpha` - decay, the daughter nuclei `._(Z)^(A)X` is moving with kinetic energy E. The total energy released if parent nuclei was at rest will be
In a nuclear reaction of `alpha` - decay, the daughter nuclei `._(Z)^(A)X` is moving with kinetic energy E. The total energy released if parent nuclei was at rest will be
A
`E(1 + 4/A)`
B
`E/A (A)`
C
`E/4(A - 4)`
D
`E(A + 4)`
Text Solution
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The correct Answer is:
To solve the problem of determining the total energy released in an alpha decay nuclear reaction, we can follow these steps:
### Step-by-Step Solution:
1. **Understanding Alpha Decay**: In alpha decay, a parent nucleus emits an alpha particle (which consists of 2 protons and 2 neutrons) and transforms into a daughter nucleus. The general reaction can be represented as:
\[
_{Z}^{A}X \rightarrow _{Z-2}^{A-4}Y + _{2}^{4}\alpha
\]
Here, \(X\) is the parent nucleus, \(Y\) is the daughter nucleus, and \(\alpha\) is the emitted alpha particle.
2. **Conservation of Energy**: The total energy released in the decay process can be expressed in terms of the mass defect and the kinetic energy of the emitted particles. The energy released \(Q\) can be given by:
\[
Q = (m_{parent} - m_{daughter} - m_{\alpha})c^2
\]
where \(m_{parent}\), \(m_{daughter}\), and \(m_{\alpha}\) are the masses of the parent nucleus, daughter nucleus, and alpha particle respectively, and \(c\) is the speed of light.
3. **Kinetic Energy of Daughter Nucleus**: The daughter nucleus \(Y\) is moving with kinetic energy \(E\). According to conservation of momentum, the momentum of the emitted alpha particle and the daughter nucleus must be equal and opposite. Thus, if \(v_{\alpha}\) is the velocity of the alpha particle and \(v_{Y}\) is the velocity of the daughter nucleus, we can write:
\[
m_{Y}v_{Y} + m_{\alpha}v_{\alpha} = 0
\]
This implies:
\[
m_{Y}v_{Y} = -m_{\alpha}v_{\alpha}
\]
4. **Relating Kinetic Energies**: The kinetic energy of the daughter nucleus can be expressed as:
\[
E = \frac{1}{2} m_{Y} v_{Y}^2
\]
and for the alpha particle:
\[
E_{\alpha} = \frac{1}{2} m_{\alpha} v_{\alpha}^2
\]
5. **Total Energy Released**: The total energy released in the decay is the sum of the kinetic energies of the daughter nucleus and the alpha particle, along with the energy equivalent of the mass defect:
\[
Q = E + E_{\alpha}
\]
6. **Final Expression**: Since we know that the kinetic energy of the daughter nucleus is \(E\), we can express the total energy released as:
\[
Q = E + \text{(kinetic energy of alpha particle)}
\]
### Conclusion:
The total energy released in the alpha decay process, when the parent nucleus is at rest, is the sum of the kinetic energy of the daughter nucleus and the kinetic energy of the emitted alpha particle, along with the energy equivalent of the mass difference.
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During alpha-decay , a nucleus decays by emitting an alpha -particle ( a helium nucleus ._2He^4 ) according to the equation ._Z^AX to ._(Z-2)^(A-4)Y+._2^4He+Q In this process, the energy released Q is shared by the emitted alpha -particle and daughter nucleus in the form of kinetic energy . The energy Q is divided in a definite ratio among the alpha -particle and the daughter nucleus . A nucleus that decays spontaneously by emitting an electron or a positron is said to undergo beta -decay .This process also involves a release of definite energy . Initially, the beta -decay was represented as ._Z^AX to ._(Z+1)^AY + e^(-)"(electron)"+Q According to this reaction, the energy released during each decay must be divided in definite ratio by the emitted e' ( beta -particle) and the daughter nucleus. While , in alpha decay, it has been found that every emitted alpha -particle has the same sharply defined kinetic energy. It is not so in case of beta -decay . The energy of emitted electrons or positrons is found to vary between zero to a certain maximum value. Wolfgang Pauli first suggested the existence of neutrinoes in 1930. He suggested that during beta -decay, a third particle is also emitted. It shares energy with the emitted beta particles and thus accounts for the energy distribution. During beta^+ decay (positron emission) a proton in the nucleus is converted into a neutron, positron and neutrino. The reaction is correctly represented as
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