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'm(1)' g of non-radioactive isotopes .(z...

`'m_(1)'` g of non-radioactive isotopes `._(z)X^(A)` are mixed with `'M_(2)'` g of the radioactive isotopes `._(z)X^(A')`. How much will the specific activity decreases ? Half-life of `._(z)X^(A')=T` Take `N_(A)` as Avagardo number.

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To solve the problem step by step, we need to calculate the specific activity before and after mixing the non-radioactive and radioactive isotopes, and then find the decrease in specific activity. ### Step 1: Define Specific Activity Before Mixing The specific activity \( A_1 \) of the radioactive isotope \( _{z}X^{A'} \) before mixing can be defined as: \[ A_1 = \frac{dN}{dt} = \lambda N \] where \( \lambda \) is the decay constant and \( N \) is the number of radioactive atoms. The decay constant \( \lambda \) can be related to the half-life \( T \) by: \[ \lambda = \frac{\ln(2)}{T} \] The number of radioactive atoms \( N \) can be calculated using the mass \( M_2 \) of the radioactive isotope and its molar mass \( A' \): \[ N = \frac{M_2}{A'} \times N_A \] where \( N_A \) is Avogadro's number. Thus, we can express the specific activity \( A_1 \) as: \[ A_1 = \frac{\ln(2)}{T} \cdot \frac{M_2}{A'} \cdot N_A \] ### Step 2: Define Specific Activity After Mixing After mixing \( m_1 \) g of non-radioactive isotopes and \( m_2 \) g of radioactive isotopes, the total mass becomes \( m_1 + m_2 \). The specific activity \( A_2 \) after mixing can be expressed as: \[ A_2 = \frac{dN_{\text{total}}}{dt} = \lambda N_{\text{total}} \] The total number of radioactive atoms \( N_{\text{total}} \) remains the same as before mixing, which is still \( N \) (since non-radioactive isotopes do not contribute to activity): \[ N_{\text{total}} = \frac{M_2}{A'} \times N_A \] Thus, the specific activity \( A_2 \) can be expressed as: \[ A_2 = \frac{\ln(2)}{T} \cdot \frac{M_2}{A'} \cdot N_A \cdot \frac{1}{m_1 + m_2} \] ### Step 3: Calculate the Decrease in Specific Activity Now, we can find the decrease in specific activity: \[ \Delta A = A_1 - A_2 \] Substituting the expressions for \( A_1 \) and \( A_2 \): \[ \Delta A = \left(\frac{\ln(2)}{T} \cdot \frac{M_2}{A'} \cdot N_A\right) - \left(\frac{\ln(2)}{T} \cdot \frac{M_2}{A'} \cdot N_A \cdot \frac{1}{m_1 + m_2}\right) \] Factoring out the common terms: \[ \Delta A = \frac{\ln(2)}{T} \cdot \frac{M_2}{A'} \cdot N_A \left(1 - \frac{1}{m_1 + m_2}\right) \] ### Final Expression for Decrease in Specific Activity Thus, the final expression for the decrease in specific activity is: \[ \Delta A = \frac{\ln(2)}{T} \cdot \frac{M_2}{A'} \cdot N_A \cdot \left(\frac{m_1}{m_1 + m_2}\right) \]

To solve the problem step by step, we need to calculate the specific activity before and after mixing the non-radioactive and radioactive isotopes, and then find the decrease in specific activity. ### Step 1: Define Specific Activity Before Mixing The specific activity \( A_1 \) of the radioactive isotope \( _{z}X^{A'} \) before mixing can be defined as: \[ A_1 = \frac{dN}{dt} = \lambda N \] ...
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