Home
Class 12
PHYSICS
Ne nucleus , the after absorbing energy ...

Ne nucleus , the after absorbing energy , decays into two `alpha` particle and an unknown nucleus . The unknown nucleus is

A

nitrogen

B

carbon

C

boron

D

oxygen

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to identify the unknown nucleus that results from the decay of a given nucleus into two alpha particles. Here’s a step-by-step breakdown of the solution: ### Step 1: Understand the decay process The problem states that a nucleus (let's denote it as N) decays into two alpha particles and an unknown nucleus (X). An alpha particle has a mass number of 4 and an atomic number of 2. ### Step 2: Define the known quantities Let’s denote the mass number of the original nucleus N as A and its atomic number as Z. According to the problem, we have: - Mass number (A) = 22 - Atomic number (Z) = 10 ### Step 3: Write the decay equation The decay can be represented as: \[ N \rightarrow 2 \alpha + X \] Where \( \alpha \) represents the alpha particles. ### Step 4: Calculate the mass number of the unknown nucleus The total mass number before decay must equal the total mass number after decay: \[ A = A_{\alpha_1} + A_{\alpha_2} + A_X \] Where: - \( A_{\alpha_1} = 4 \) (mass number of the first alpha particle) - \( A_{\alpha_2} = 4 \) (mass number of the second alpha particle) - \( A_X \) is the mass number of the unknown nucleus. Substituting the values: \[ 22 = 4 + 4 + A_X \] \[ 22 = 8 + A_X \] \[ A_X = 22 - 8 = 14 \] ### Step 5: Calculate the atomic number of the unknown nucleus Similarly, the total atomic number before decay must equal the total atomic number after decay: \[ Z = Z_{\alpha_1} + Z_{\alpha_2} + Z_X \] Where: - \( Z_{\alpha_1} = 2 \) (atomic number of the first alpha particle) - \( Z_{\alpha_2} = 2 \) (atomic number of the second alpha particle) - \( Z_X \) is the atomic number of the unknown nucleus. Substituting the values: \[ 10 = 2 + 2 + Z_X \] \[ 10 = 4 + Z_X \] \[ Z_X = 10 - 4 = 6 \] ### Step 6: Identify the unknown nucleus Now we have: - Mass number \( A_X = 14 \) - Atomic number \( Z_X = 6 \) We can now identify the unknown nucleus. The nucleus with atomic number 6 and mass number 14 is Carbon (C). ### Conclusion The unknown nucleus is Carbon (C).

To solve the problem, we need to identify the unknown nucleus that results from the decay of a given nucleus into two alpha particles. Here’s a step-by-step breakdown of the solution: ### Step 1: Understand the decay process The problem states that a nucleus (let's denote it as N) decays into two alpha particles and an unknown nucleus (X). An alpha particle has a mass number of 4 and an atomic number of 2. ### Step 2: Define the known quantities Let’s denote the mass number of the original nucleus N as A and its atomic number as Z. According to the problem, we have: - Mass number (A) = 22 ...
Promotional Banner

Similar Questions

Explore conceptually related problems

A nucleus ._n^ m X emits one alpha- particle and two beta- particles. The resulting nucleus is

An unknown stable nuclide after absorbing a neutron emits an electron, and the new nuclide splits spontaneously into two alpha particles. The unknown nuclide is :

In Rutherford experiment alpha – particles are scattered by nucleus having change 100 e^(-) Initial kinetic energy of alpha - particles is 6 MeV . The size of the nucleus is

which a U^(238) nucleus original at rest , decay by emitting an alpha particle having a speed u , the recoil speed of the residual nucleus is

which a U^(238) nucleus original at rest , decay by emitting an alpha particle having a speed u , the recoil speed of the residual nucleus is

A stationary radioactive nucleus of mass 210 units disintegrates into an alpha particle of mass 4 units and residual nucleus of mass 206 units. If the kinetic energy of the alpha particle is E, then the kinetic energy of the residual nucleus is

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

Initially the nucleus of radium 226 is at rest. It decays due to which and alpha particle and the nucleus of radon are created. The released energy during the decay is 4.87 Mev, which appears as the kinetic energy of the two resulted particles [m_(alpha)=4.002"amu",m_("Rn")=22.017"amu"] Kinetic energies of alpha particle & radon nucleus are respectively

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. The beta particles (positron) are emitted with different kinetic energies because

A uranium nucleus U-238 of atomic number 92 emits two alpha - particles and two beta -particles and trasnforms into a thorium nucleus. What is the mass number and atomic number of the thorium nucleus so produced?