The nuclei of 137 Cs decay by the emission of β - particles with a half life of 30.08 years. The activity (in units of disintegrations per second or Bq) of a 1 mg source of 137 Cs, prepared on January 1, 1980, as measured on January 1, 2021 is closest to
1.24 × 10 9
Let's calculate the radioactive activity of the Cesium-137 sample. The activity decreases over time due to radioactive decay. We are given the half-life, the initial mass of the source, and the time elapsed since its preparation.
Here are the given parameters for the Cesium-137 ($^{137}$Cs) decay:
First, we need to find the time elapsed ($t$) between the preparation date and the measurement date.
Time elapsed ($t$) = Measurement Year - Preparation Year
$t = 2021 - 1980 = 41$ years
The decay constant ($\lambda$) is related to the half-life by the formula:
$\lambda = \frac{\ln(2)}{T_{1/2}}$
To calculate the activity in Becquerels (Bq), which is disintegrations per second, we need the decay constant in units of s-1. First, let's find $\lambda$ in year-1:
$\lambda_{year} = \frac{0.6931}{30.08 \text{ years}} \approx 0.02304 \text{ year}^{-1}$
Now, convert years to seconds (1 year $\approx$ 365.25 days $\times$ 24 hours/day $\times$ 3600 seconds/hour $\approx$ 31,557,600 seconds):
$\lambda_{sec} = \frac{0.6931}{30.08 \text{ years}} \times \frac{1 \text{ year}}{31,557,600 \text{ seconds}}$
$\lambda_{sec} = \frac{0.6931}{949,626,480} \text{ s}^{-1} \approx 7.30 \times 10^{-10} \text{ s}^{-1}$
We need to find the initial number of $^{137}$Cs nuclei ($N_0$) in 1 mg of the source. We can use the molar mass of $^{137}$Cs (approximately 137 g/mol) and Avogadro's number ($N_A = 6.022 \times 10^{23}$ mol-1).
Initial mass ($m$) = 1 mg = $1 \times 10^{-3}$ g
Molar mass of $^{137}$Cs = 137 g/mol
Number of moles = $\frac{\text{Mass}}{\text{Molar mass}} = \frac{1 \times 10^{-3} \text{ g}}{137 \text{ g/mol}}$
$N_0 = \text{Number of moles} \times N_A = \left(\frac{1 \times 10^{-3}}{137}\right) \times (6.022 \times 10^{23})$
$N_0 = \frac{6.022 \times 10^{20}}{137} \approx 4.396 \times 10^{18}$ nuclei
The initial activity ($A_0$) is given by $A_0 = \lambda_{sec} N_0$.
$A_0 = (7.30 \times 10^{-10} \text{ s}^{-1}) \times (4.396 \times 10^{18})$
$A_0 \approx 3.21 \times 10^9$ Bq
The activity ($A_t$) at a time $t$ after the initial time is given by the radioactive decay formula:
$A_t = A_0 e^{-\lambda_{year} t}$
We calculated $A_0 \approx 3.21 \times 10^9$ Bq, $\lambda_{year} \approx 0.02304$ year-1, and $t = 41$ years.
$\lambda_{year} t \approx 0.02304 \times 41 \approx 0.94464$
$A_t \approx (3.21 \times 10^9) e^{-0.94464}$
Calculate $e^{-0.94464}$:
$e^{-0.94464} \approx 0.3888$
Now, calculate $A_t$:
$A_t \approx (3.21 \times 10^9) \times 0.3888$
$A_t \approx 1.248 \times 10^9$ Bq
The calculated activity on January 1, 2021, is approximately $1.248 \times 10^9$ Bq.
Let's compare our calculated value with the given options:
Our calculated value, $1.248 \times 10^9$, is closest to $1.24 \times 10^9$.
The activity of the Cesium-137 source on January 1, 2021, is closest to $1.24 \times 10^9$ disintegrations per second (Bq).
The Q - value of the α - decay of 232 Th to the ground state of 228 Ra is 4082 keV. The maximum possible kinetic energy of the α - particle is closest to
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