Respuesta :
The equation of radioactive decay and half-life time allows to find the answers are:
a) The activity is valid is λ = 3.85 10-4 s⁺¹ and is constant for any time
b) the amount of matter in atom X is 1.2 10⁻¹⁶ mol
Given parameters
- The half-life time tau = 30 min = 1800 s
- The amount of material n = 2 10⁻¹² mol
To find
- Activity
- The particles after a time t = 7 h
Radioactivity is a process by which heavy and unstable atoms can decay into other lighter and more stable atoms. There are three main emission processes: alpha particle, beta particle and gamma rays.
All processes can be characterized by a probabilistic decay described by the expressions
[tex]N = N_0 \ e^{- \lan \ t}[/tex]
don N and N₀ is the current and initial particle number, lamba the decay constant and t the time.
The half-life time is a very useful quantity defined as the time that half of the radioactive material decays
[tex]T_ \frac{1}{2} = \frac{ln 2}{\lambda}[/tex]
λ = [tex]\frac{ln 2}{ T_\frac{1}{2} }[/tex]
λ = [tex]\frac{ln \ 2}{1800}[/tex]
λ = 3.85 10⁻⁴ s⁻¹
This value of the activity does not depend on the time that passes, it is a property of the material
b) Let's find the particle number that remains after t = 7 h
t = 7 h ([tex]\frac{3600s }{1 h}[/tex]) = 2.52 10⁴ s
We look for the initial quantity of matter with a direct rule of proportions. If 1 mole of matter is avogadro's number 6.022 1023, how much matter is 210-12 mole
# _particles = 2 10⁻¹² mol (6.022 10²³ particles /1 mol)
# _particles= 1.2 10¹² particles
We use the initial expression
N = [tex]1.2 \ 10^{12} \ e^{- 3.85 \ 10^{-4} \ 2.52 \ 10^4 }[/tex]
N = 7,339 10⁷ particles
Let's reduce this number to quantity of materia
n = 7.339 10⁷ particles ( [tex]\frac{1 mol}{6.022 \ 10^{23} \ particles }[/tex] )
n = 1.219 10⁻¹⁶ mol
In conclusion, using the radioactive decay and half-life time equations we can find the answers are:
a) The activity is valid and is constant for any time λ = 3.85 10⁻⁴ s⁻¹
b) the amount of matter in atom X is 1.2 10⁻¹⁶ mol
Learn more about radioactivity here:
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