Problem 103
Question
A sample of radioactive substance gave 630 counts per minute and 610 counts per minute at times differing by 1 hour. The decay constant \((\lambda)\) in \(\min ^{-1}\) is given by (a) \(\lambda=\frac{630}{610} \times 60\) (b) \(\mathrm{e}^{60 \mathrm{~A}}=\frac{630}{610}\) (c) \(\lambda=\frac{2.303}{60} \log \frac{610}{630}\) (d) \(\lambda=\frac{2.303}{60} \times \frac{630}{610}\)
Step-by-Step Solution
Verified Answer
The decay constant is given by option (c) \( \lambda=\frac{2.303}{60} \log \frac{630}{610} \).
1Step 1: Identify the decay formula
The decay of a radioactive substance over time can be described using the equation: \[ N(t) = N_0 e^{- ext{decay constant} imes t} \]where \( N(t) \) is the amount at time \( t \), and \( N_0 \) is the initial quantity. The decay constant can be expressed in terms of time in minutes when we know the initial and subsequent counts.
2Step 2: Formulate the decay equation for this problem
Given that the counts reduce from 630 to 610 in 60 minutes, the decay equation becomes:\[ 610 = 630 e^{- ext{decay constant} imes 60} \]
3Step 3: Solve the decay constant equation
Rearrange the equation to solve for the decay constant:1. Divide both sides by 630: \[ \frac{610}{630} = e^{- ext{decay constant} imes 60} \]2. Take the natural logarithm of both sides: \[ ext{ln}\left(\frac{610}{630}\right) = - ext{decay constant} imes 60 \]
4Step 4: Isolate the decay constant
Solve for the decay constant:\[ ext{decay constant} = -rac{1}{60} imes ext{ln}\left(\frac{610}{630}\right) \]
5Step 5: Convert natural logarithm to common logarithm
Apply the rule of logarithms to convert it to a base-10 logarithm using:\[ ext{ln}(x) = 2.303 imes ext{log}_{10}(x) \]Therefore:\[ ext{decay constant} = -rac{1}{60} imes 2.303 imes ext{log}_{10}\left(\frac{610}{630}\right) \]Simplifying further, it becomes:\[ ext{decay constant} = rac{2.303}{60} imes ext{log}_{10}\left(\frac{630}{610}\right) \]
6Step 6: Match the derived formula with given options
The correct option corresponding to the decay constant formula we derived is (c) \( \lambda=\frac{2.303}{60} \log \frac{630}{610} \).
Key Concepts
Decay ConstantRadioactivity EquationHalf-Life Computation
Decay Constant
Imagine you have a shrinking snowball. Every minute, it shrinks at a predictable rate. The decay constant in radioactivity is similar, representing the rate at which a radioactive substance decays.
In mathematical terms, it shows how quickly the substance is losing particles. In the equation, \( N(t) = N_0 e^{-\lambda \times t} \), the decay constant, \( \lambda \), tells us how fast \( N \) reduces from \( N_0 \) over time \( t \).
In mathematical terms, it shows how quickly the substance is losing particles. In the equation, \( N(t) = N_0 e^{-\lambda \times t} \), the decay constant, \( \lambda \), tells us how fast \( N \) reduces from \( N_0 \) over time \( t \).
- \( \lambda \) is the decay constant.
- Higher \( \lambda \) means faster decay.
- Units for \( \lambda \) often match the time unit used, like per minute (\( \min^{-1} \)).
Radioactivity Equation
The radioactivity equation is like a magical formula that lets us see into the future of decay. It helps predict how much of a substance remains after a certain time period.
This formula involves an exponential function because radioactivity diminishes over time, not disappearing all at once. The defining equation is:
This formula involves an exponential function because radioactivity diminishes over time, not disappearing all at once. The defining equation is:
- \( N(t) = N_0 e^{-\lambda \times t} \)
- \( N(t) \) is the remaining amount after time \( t \).
- \( N_0 \) is the original quantity.
- \( e \) is the base of the natural logarithm (approximately 2.718).
Half-Life Computation
The half-life of a substance is the time it takes for half of it to decay. It's a handy concept because it gives a clear picture of how long a substance stays active. Mathematically, it's calculated using the decay constant. The relationship between half-life and the decay constant is:
In our exercise, deriving the decay constant led us one step closer to understanding this half-life, even though the computation focused on \( \lambda \) itself, our understanding of how things decay is based on this core concept.
- \( t_{1/2} = \frac{\ln(2)}{\lambda} \)
- Here, \( \ln(2) \) approximates to 0.693.
In our exercise, deriving the decay constant led us one step closer to understanding this half-life, even though the computation focused on \( \lambda \) itself, our understanding of how things decay is based on this core concept.
Other exercises in this chapter
Problem 100
What weight of \(\mathrm{C}^{14}\) will have radioactivity one curie if \(\lambda\) (disintegration constant) is \(4.4 \times 10^{-12} \mathrm{sec}^{-1}\) ? (a)
View solution Problem 101
Half-life period of the radioactive element \(X\) is 10 hours. Amount of \(X\) left in the 11 th hour starting with one \(m o l X\) is (a) \((1 / 2)^{1 / 10}\)
View solution Problem 104
In one type of mutual annihilation of an electron and a positron, three \gamma-ray photons are produced. If each photon has an energy of \(0.3407 \mathrm{MeV}\)
View solution Problem 105
Assuming the age of the earth to be \(10^{10}\) years, what fraction of the original amount of \({ }_{92} \mathrm{U}^{218}\) is still in existence on earth \(\l
View solution