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The radionuclide .^(56)Mn is being produ...

The radionuclide `.^(56)Mn` is being produced in a cyclontron at a constant rate `P` by bombarding a manganese target with deutrons. `.^(56)Mn` has a half-life of `2.5 h` and the target contains large numbers of only the stable manganese isotopes `.^(56)Mn`. The reaction that produces `^(56)Mn` is
`.^(56)Mn` +`d` `rarr .^(56)Mn` +`p`
After being bombarded for a long time, the activity of `.^(56)Mn` becomes constant, equal to `13.86 xx 10^(10) s^(-1)`. (Use `l n2=0.693`, Avagadro number` =6 xx 10^(23)`, atomic weight of `.^(56)Mn`=`56 g mol^(-1))`.
After the activity of `.^(56)Mn` becomes constant, number of `.^(56)Mn` nuclei present in the target is equal to .

A

`5xx10^(11)`

B

`20xx10^(11)`

C

`1.2xx10^(14)`

D

`1.8xx10^(15)`

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The correct Answer is:
To solve the problem, we need to find the number of nuclei of the radionuclide \(^{56}\text{Mn}\) present in the target after the activity becomes constant. We will use the relationship between the activity, decay constant, and the number of nuclei. ### Step-by-step Solution: 1. **Understanding the Equilibrium Condition**: At equilibrium, the rate of production of \(^{56}\text{Mn}\) (denoted as \(P\)) is equal to the rate of decay of \(^{56}\text{Mn}\). This can be expressed mathematically as: \[ P = \lambda N \] where \(N\) is the number of nuclei and \(\lambda\) is the decay constant. 2. **Finding the Decay Constant**: The decay constant \(\lambda\) is related to the half-life (\(t_{1/2}\)) of the radionuclide by the formula: \[ \lambda = \frac{\ln 2}{t_{1/2}} \] Given that the half-life of \(^{56}\text{Mn}\) is \(2.5\) hours, we first convert this into seconds: \[ t_{1/2} = 2.5 \text{ hours} = 2.5 \times 3600 \text{ seconds} = 9000 \text{ seconds} \] Now, substituting this value into the decay constant formula: \[ \lambda = \frac{0.693}{9000} \approx 7.7 \times 10^{-5} \text{ s}^{-1} \] 3. **Substituting the Activity**: The activity \(A\) (which is given as \(13.86 \times 10^{10} \text{ s}^{-1}\)) can be substituted into the equilibrium equation: \[ N = \frac{P}{\lambda} \] Therefore: \[ N = \frac{13.86 \times 10^{10}}{7.7 \times 10^{-5}} \] 4. **Calculating the Number of Nuclei**: Performing the calculation: \[ N \approx \frac{13.86 \times 10^{10}}{7.7 \times 10^{-5}} \approx 1.80 \times 10^{15} \] 5. **Final Answer**: Thus, the number of \(^{56}\text{Mn}\) nuclei present in the target after the activity becomes constant is approximately: \[ N \approx 1.8 \times 10^{15} \]

To solve the problem, we need to find the number of nuclei of the radionuclide \(^{56}\text{Mn}\) present in the target after the activity becomes constant. We will use the relationship between the activity, decay constant, and the number of nuclei. ### Step-by-step Solution: 1. **Understanding the Equilibrium Condition**: At equilibrium, the rate of production of \(^{56}\text{Mn}\) (denoted as \(P\)) is equal to the rate of decay of \(^{56}\text{Mn}\). This can be expressed mathematically as: \[ P = \lambda N ...
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The radionuclide .^(56)Mn is being produced in a cyclontron at a constant rate P by bombarding a manganese target with deutrons. .^(56)Mn has a half-life of 2.5 h and the target contains large numbers of only the stable manganese isotopes .^(56)Mn . The reaction that produces .^(56)Mn is .^(56)Mn +d rarr .^(56)Mn +p After being bombarded for a long time, the activity of .^(56)Mn becomes constant, equal to 13.86 xx 10^(10) s^(-1) . (Use 1 n2=0.693 , Avagardo number =6 xx 10^(2) , atomic weight of .^(56)Mn=56 g mol^(-1) ). After a long time bombardment, number .^(56)Mn nuclei present in the target depends upon.

The radionuclide .^(56)Mn is being produced in a cyclontron at a constant rate P by bombarding a manganese target with deutrons. .^(56)Mn has a half-life of 2.5 h and the target contains large numbers of only the stable manganese isotopes .^(56)Mn . The reaction that produces .^(56)Mn is .^(56)Mn +d rarr .^(56)Mn +p After being bombarded for a long time, the activity of .^(56)Mn becomes constant, equal to 13.86 xx 10^(10) s^(-1) . (Use 1 n2=0.693 , Avagardo number =6 xx 10^(2) , atomic weight of .^(56)Mn=56 g mol^(-1) ). After a long time bombardment, number .^(56)Mn nuclei present in the target depends upon. (i) number of Mn nuclei present at the start of the process. (ii) half life of Mn. (iii) constant rate of production P

The radionuclide .^(56)Mn is being produced in a cyclontron at a constant rate P by bombarding a manganese target with deutrons. .^(56)Mn has a half-life of 2.5 h and the target contains large numbers of only the stable manganese isotopes .^(56)Mn . The reaction that produces .^(56)Mn is .^(56)Mn +d rarr .^(56)Mn +p After being bombarded for a long time, the activity of .^(56)Mn becomes constant, equal to 13.86 xx 10^(10) s^(-1) . (Use 1 n2=0.693 , Avagardo number =6 xx 10^(2) , atomic weight of .^(56)Mn=56 g mol^(-1) ). At what constant rate P, .^(56)Mn nuclei are being produced in the cyclontron during the bombardment?

The radionuclide .^(56)Mn is being produced in a cyclontron at a constant rate P by bombarding a manganese target with deutrons. .^(56)Mn has a half-life of 2.5 h and the target contains large numbers of only the stable manganese isotopes .^(56)Mn . The reaction that produces .^(56)Mn is .^(56)Mn +d rarr .^(56)Mn +p After being bombarded for a long time, the activity of .^(56)Mn becomes constant, equal to 13.86 xx 10^(10) s^(-1) . (Use 1 n2=0.693 , Avagardo number =6 xx 10^(23) , atomic weight of .^(56)Mn=56 g mol^(-1) ). At what constant rate P, .^(56)Mn nuclei are being produced in the cyclotron during the bombardment?

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