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A nucleus kept at rest in free space, br...

A nucleus kept at rest in free space, brakes up into smaller nuclei of masses `'m'` and `'2m'`. Total energy generated in this fission is `E`. The bigger part is radioactive, emits five gamma ray photons in the direction opposite to its velocity and finally comes torest. `["Given" h=6.6xx10^(-34)Js,m=1xx10^(-26)Kg,E= 3.63xx10^(-8) mc^(2), C=3xx10^(8)m//s)`
Fractional loss of mass in the fission is

A

`1.21 xx10^(-8)`

B

`2.56xx10^(-8)`

C

1.73xx10^(-8)`

D

`3.52 xx 10^(-8)`

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The correct Answer is:
To solve the problem of fractional loss of mass during the fission of a nucleus, we can follow these steps: ### Step 1: Understanding the Problem We have a nucleus that breaks into two smaller nuclei of masses `m` and `2m`. The total energy generated in this fission is given as `E`. The larger nucleus emits five gamma ray photons and comes to rest. We need to find the fractional loss of mass during this fission process. ### Step 2: Relate Energy to Mass Loss According to the mass-energy equivalence principle, the change in mass (Δm) can be related to the energy (E) generated during the fission using the equation: \[ \Delta m c^2 = E \] From this, we can express the change in mass as: \[ \Delta m = \frac{E}{c^2} \] ### Step 3: Substitute the Given Energy We are given that: \[ E = 3.63 \times 10^{-8} m c^2 \] Substituting this into our equation for Δm gives: \[ \Delta m = \frac{3.63 \times 10^{-8} m c^2}{c^2} \] The \( c^2 \) terms cancel out: \[ \Delta m = 3.63 \times 10^{-8} m \] ### Step 4: Calculate the Total Mass After Fission The total mass before fission is the mass of the original nucleus, which is \( 3m \) (since it breaks into masses \( m \) and \( 2m \)). After the fission, the total mass is: \[ \text{Total mass after fission} = m + 2m - \Delta m = 3m - \Delta m \] ### Step 5: Calculate Fractional Loss of Mass The fractional loss of mass (F) can be calculated using the formula: \[ F = \frac{\Delta m}{\text{Initial mass}} \] Substituting the values we have: \[ F = \frac{\Delta m}{3m} = \frac{3.63 \times 10^{-8} m}{3m} \] The \( m \) terms cancel out: \[ F = \frac{3.63 \times 10^{-8}}{3} \] Calculating this gives: \[ F = 1.21 \times 10^{-8} \] ### Final Answer The fractional loss of mass in the fission is: \[ F = 1.21 \times 10^{-8} \] ---

To solve the problem of fractional loss of mass during the fission of a nucleus, we can follow these steps: ### Step 1: Understanding the Problem We have a nucleus that breaks into two smaller nuclei of masses `m` and `2m`. The total energy generated in this fission is given as `E`. The larger nucleus emits five gamma ray photons and comes to rest. We need to find the fractional loss of mass during this fission process. ### Step 2: Relate Energy to Mass Loss According to the mass-energy equivalence principle, the change in mass (Δm) can be related to the energy (E) generated during the fission using the equation: \[ \Delta m c^2 = E \] ...
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A nucleus kept at rest in free space, brakes up into smaller nuclei of masses 'm' and '2m' . Total energy generated in this fission is E . The bigger part is radioactive, emits five gamma ray photons in the direction opposite to its velocity and finally comes torest. ["Given" h=6.6xx10^(-34)Js,m=1xx10^(-26)Kg,E= 3.63xx10^(-8) mc^(2), C=3xx10^(8)m//s) The wavelength of the gamma ray is

A nucleus kept at rest in free space, brakes up into smaller nuclei of masses 'm' and '2m' . Total energy generated in this fission is E . The bigger part is radioactive, emits five gamma ray photons in the direction opposite to its velocity and finally comes torest. ["Given" h=6.6xx10^(-34)Js,m=1xx10^(-26)Kg , E= 3.63xx10^(-8) mc^(2), C=3xx10^(8)m//s) The wavelength of the gamma ray is

A nucleus kept at rest in free space, brakes up into smaller nuclei of masses 'm' and '2m' . Total energy generated in this fission is E . The bigger part is radioactive, emits five gamma ray photons in the direction opposite to its velocity and finally comes torest. ["Given" h=6.6xx10^(-34)Js,m=1xx10^(-26)Kg , E= 3.63xx10^(-8) mc^(2), C=3xx10^(8)m//s) Velocity of small daughter nucleus is

A nucleus kept at rest in free space, brakes up into smaller nuclei of masses 'm' and '2m' . Total energy generated in this fission is E . The bigger part is radioactive, emits five gamma ray photons in the direction opposite to its velocity and finally comes torest. ["Given" h=6.6xx10^(-34)Js,m=1xx10^(-26)Kg,E= 3.63xx10^(-8) mc^(2), C=3xx10^(8)m//s) Velocity of small daughter nucleus is

The de Broglie wavelength of an electron with kinetic energy 120 e V is ("Given h"=6.63xx10^(-34)Js,m_(e)=9xx10^(-31)kg,1e V=1.6xx10^(-19)J)

If de Broglie wavelength of an electron is 0.5467 Å, find the kinetic energy of electron in eV. Given h=6.6xx10^(-34) Js , e= 1.6xx10^(-19) C, m_e=9.11xx10^(-31) kg.

What is the (a) momentum (b) speed and (c) de-Broglie wavelength of an electron with kinetic energy of 120 eV. Given h=6.6xx10^(-34)Js, m_(e)=9xx10^(-31)kg , 1eV=1.6xx10^(-19)J .

Calculate the (a) momentum and (b) de-Broglie wavelength of the electrons accelerated through a potential difference of 56V. Given, h=6.63xx10^(-34)Js, m_(e)=9.1xx10^(-31)kg, e=1.6xx10^(-19)C .

A neutron breaks into a proton and electorn. Calculate the eenrgy produced in this reaction in m_(e) = 9 xx 10^(-31) kg, m_(p) = 1.6725 xx 10^(-27) kg, m_(n) = 1.6747 xx 10^(-27) kg, c = 3xx10^(8)m//sec .

For given enegy, corresponding wavelength will be E = 3.03 xx 10^(-19) Joules (h = 6.6 xx 10^(-34) j X sec., C = 3 xx 10^(8) m/sec

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