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Radioactiv edecay will occur as follows ...

Radioactiv edecay will occur as follows
`overset(220)86Rnrarroverset(216)84PO + overset(4)2He ` Half life =55s
`overset(216)84Poarroverset(212)82Pb + overset(4)2He ` Half life =0.66s
`overset(812)82Pbrarroverset(212)82Bi + overset(0)-1e ` Half life =10.6 s
If a certain mass of radon (Rn=220) is allowed to decay in a certain container,then after 5 minutes the element with the greater mass will be

A

radon

B

polonium

C

lead

D

bismuth

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The correct Answer is:
To solve the problem, we need to analyze the decay of the radioactive elements step by step and determine which element will have the greatest mass after 5 minutes (300 seconds). ### Step 1: Determine the number of half-lives for each element First, we need to calculate how many half-lives each element undergoes in 5 minutes (300 seconds). 1. **Radon (Rn-220)**: Half-life = 55 seconds \[ \text{Number of half-lives} = \frac{300 \text{ seconds}}{55 \text{ seconds}} \approx 5.45 \text{ half-lives} \] 2. **Polonium (Po-216)**: Half-life = 0.66 seconds \[ \text{Number of half-lives} = \frac{300 \text{ seconds}}{0.66 \text{ seconds}} \approx 454.55 \text{ half-lives} \] 3. **Lead (Pb-212)**: Half-life = 10.6 seconds \[ \text{Number of half-lives} = \frac{300 \text{ seconds}}{10.6 \text{ seconds}} \approx 28.30 \text{ half-lives} \] ### Step 2: Calculate the remaining mass for each element Assuming we start with a mass \( M_0 \) of Radon (Rn-220), we can calculate the remaining mass after the decay for each element. 1. **Radon (Rn-220)**: \[ M_{\text{Rn}} = M_0 \left(\frac{1}{2}\right)^{5.45} \approx M_0 \cdot 0.028 \] 2. **Polonium (Po-216)**: Since Polonium is produced from Radon, we need to calculate how much Polonium is produced before it decays. The amount of Polonium produced can be approximated using the decay of Radon: \[ M_{\text{Po}} \approx M_0 - M_{\text{Rn}} \approx M_0 - M_0 \cdot 0.028 \approx M_0 \cdot 0.972 \] However, this will also decay into Lead, so we need to account for that as well. 3. **Lead (Pb-212)**: Lead is produced from the decay of Polonium. The amount of Lead produced can be calculated from the decay of Polonium: \[ M_{\text{Pb}} \approx M_{\text{Po}} \left(1 - \left(\frac{1}{2}\right)^{454.55}\right) \approx M_{\text{Po}} \approx M_0 \cdot 0.972 \] Since the decay of Polonium is very rapid, almost all of it will convert to Lead. ### Step 3: Compare the masses Now we need to compare the remaining masses of Radon, Polonium, and Lead after 5 minutes. - **Remaining mass of Radon**: \( M_{\text{Rn}} \approx M_0 \cdot 0.028 \) - **Remaining mass of Polonium**: \( M_{\text{Po}} \) will be very small due to its rapid decay. - **Mass of Lead**: Since Polonium decays rapidly into Lead, the mass of Lead will be significant. ### Conclusion After 5 minutes, the element with the greatest mass will be **Lead (Pb-212)**, as it is produced from the decay of Polonium and has a much slower decay rate compared to Polonium.

To solve the problem, we need to analyze the decay of the radioactive elements step by step and determine which element will have the greatest mass after 5 minutes (300 seconds). ### Step 1: Determine the number of half-lives for each element First, we need to calculate how many half-lives each element undergoes in 5 minutes (300 seconds). 1. **Radon (Rn-220)**: Half-life = 55 seconds \[ \text{Number of half-lives} = \frac{300 \text{ seconds}}{55 \text{ seconds}} \approx 5.45 \text{ half-lives} ...
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Scientists are working hard to develop nuclear fusion reactor Nuclei of heavy hydrogen, _(1)^(2)H , known as deuteron and denoted by D , can be thought of as a candidate for fusion rector . The D-D reaction is _(1)^(2) H + _(1)^(2) H rarr _(2)^(1) He + n+ energy. In the core of fusion reactor, a gas of heavy hydrogen of _(1)^(2) H is fully ionized into deuteron nuclei and electrons. This collection of _1^2H nuclei and electrons is known as plasma . The nuclei move randomly in the reactor core and occasionally come close enough for nuclear fusion to take place. Usually , the temperature in the reactor core are too high and no material will can be used to confine the to plasma for a time t_(0) before the particles fly away from the core. If n is the density (number volume ) of deuterons , the product nt_(0) is called Lawson number. In one of the criteria , a reactor is termed successful if Lawson number is greater then 5 xx 10^(14) s//cm^(2) it may be helpfull to use the following boltzmann constant lambda = 8.6 xx 10^(-5)eV//k, (e^(2))/(4 pi s_(0)) = 1.44 xx 10^(-9) eVm Assume that two deuteron nuclei in the core of fusion reactor at temperature energy T are moving toward each other, each with kinectic energy 1.5 kT , when the seperation between them is large enough to neglect coulomb potential energy . Also neglate any interaction from other particle in the core . The minimum temperature T required for them to reach a separation of 4 xx 10^(-15) m is in the range

Scientists are working hard to develop nuclear fusion reactor Nuclei of heavy hydrogen, _(1)^(2)H , known as deuteron and denoted by D , can be thought of as a candidate for fusion rector . The D-D reaction is _(1)^(2) H + _(1)^(2) H rarr _(2)^(1) He + n+ energy. In the core of fusion reactor, a gas of heavy hydrogen of _(1)^(2) H is fully ionized into deuteron nuclei and electrons. This collection of _1^2H nuclei and electrons is known as plasma . The nuclei move randomly in the reactor core and occasionally come close enough for nuclear fusion to take place. Usually , the temperature in the reactor core are too high and no material will can be used to confine the to plasma for a time t_(0) before the particles fly away from the core. If n is the density (number volume ) of deuterons , the product nt_(0) is called Lawson number. In one of the criteria , a reactor is termed successful if Lawson number is greater then 5 xx 10^(14) s//cm^(2) it may be helpfull to use the following boltzmann constant lambda = 8.6 xx 10^(-5)eV//k, (e^(2))/(4 pi s_(0)) = 1.44 xx 10^(-9) eVm In the core of nucleus fusion reactor , the gas become plasma because of

Scientists are working hard to develop nuclear fusion reactor Nuclei of heavy hydrogen, _(1)^(2)H , known as deuteron and denoted by D , can be thought of as a candidate for fusion rector . The D-D reaction is _(1)^(2) H + _(1)^(2) H rarr _(2)^(1) He + n+ energy. In the core of fusion reactor, a gas of heavy hydrogen of _(1)^(2) H is fully ionized into deuteron nuclei and electrons. This collection of _1^2H nuclei and electrons is known as plasma . The nuclei move randomly in the reactor core and occasionally come close enough for nuclear fusion to take place. Usually , the temperature in the reactor core are too high and no material will can be used to confine the to plasma for a time t_(0) before the particles fly away from the core. If n is the density (number volume ) of deuterons , the product nt_(0) is called Lawson number. In one of the criteria , a reactor is termed successful if Lawson number is greater then 5 xx 10^(14) s//cm^(2) it may be helpfull to use the following boltzmann constant lambda = 8.6 xx 10^(-5)eV//k, (e^(2))/(4 pi s_(0)) = 1.44 xx 10^(-9) eVm In the core of nucleus fusion reactor , the gas become plasma because of

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