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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 `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?

A

`2xx10^(11) "nuclei"//s`

B

`13.86xx10^(10) "nuclei"//s`

C

`9.6xx10^(10) "nuclei"//s`

D

`6.93xx10^(10) "nuclei"//s`

Text Solution

AI Generated Solution

The correct Answer is:
To find the constant rate \( P \) at which \( ^{56}Mn \) nuclei are being produced in the cyclotron, we can use the relationship between the activity of a radioactive substance and its decay constant. Here’s a step-by-step solution: ### Step 1: Understand the relationship between activity, decay constant, and number of nuclei The activity \( A \) of a radioactive substance is given by the formula: \[ A = \lambda N \] where: - \( A \) is the activity (in decays per second), - \( \lambda \) is the decay constant (in \( s^{-1} \)), - \( N \) is the number of radioactive nuclei present. ### Step 2: Calculate the decay constant \( \lambda \) The decay constant \( \lambda \) is related to the half-life \( T_{1/2} \) by the formula: \[ \lambda = \frac{0.693}{T_{1/2}} \] Given that the half-life \( T_{1/2} \) of \( ^{56}Mn \) is 2.5 hours, we first convert this into seconds: \[ T_{1/2} = 2.5 \, \text{hours} \times 3600 \, \text{seconds/hour} = 9000 \, \text{seconds} \] Now, we can calculate \( \lambda \): \[ \lambda = \frac{0.693}{9000 \, \text{s}} \approx 7.7 \times 10^{-5} \, \text{s}^{-1} \] ### Step 3: Use the constant activity to find \( N \) The problem states that the activity \( A \) of \( ^{56}Mn \) is \( 13.86 \times 10^{10} \, s^{-1} \). We can rearrange the activity formula to solve for \( N \): \[ N = \frac{A}{\lambda} \] Substituting the values we have: \[ N = \frac{13.86 \times 10^{10} \, s^{-1}}{7.7 \times 10^{-5} \, s^{-1}} \approx 1.80 \times 10^{15} \, \text{nuclei} \] ### Step 4: Relate the production rate \( P \) to the decay rate At equilibrium, the rate of production \( P \) of \( ^{56}Mn \) is equal to the rate of decay, which is equal to the activity \( A \): \[ P = A = 13.86 \times 10^{10} \, s^{-1} \] ### Final Answer Thus, the constant rate \( P \) at which \( ^{56}Mn \) nuclei are being produced in the cyclotron is: \[ P = 13.86 \times 10^{10} \, \text{s}^{-1} \] ---
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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 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 .

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

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