Analyzing the Setup
Let's start by looking at the initial conditions
At time t=0, the activities of both radioactive substances, A and B, are perfectly equal. We can call this initial activity R0.
Now, according to the radioactive decay law, the activity at any time t follows an exponential curve. It is given by the master equation:
where λ is the decay constant. This equation tells us exactly how fast a radioactive sample is disintegrating at any given moment.
Finding the Decay Constant of A
We are given a crucial piece of information: the half-life of substance A is ln2
We know the standard formula relating half-life and the decay constant is:
Equating this to the given value, we get:
Solving this simple equation, we easily find that the decay constant for A, λA, is exactly 1.
The Ratio of Activities
Next, let's find the ratio of their activities at any time t
By dividing RB by RA, the initial activity R0 beautifully cancels out:
RA(t)RB(t)=R0e−λAtR0e−λBt
Using the fundamental properties of exponents, we can combine the terms in the numerator and denominator:
RA(t)RB(t)=e−(λB−λA)t
Comparing Exponents and Final Calculation
The problem states this ratio decreases according to e−3t
By comparing the exponents of our derived ratio and the given ratio, we can clearly see that:
Since we already calculated λA=1, let's substitute it here. This gives us:
So, substance B decays four times faster than A! Finally, we need to find the half-life of substance B. Using the half-life formula again, (T1/2)B is λBln2. Substituting λB=4, we get our final answer: