00:01
In this problem, we're going to use the concepts of activity, the half -life, and the decay constant, along with their equation representations, to figure out the half -life and the decay constant, as well as the activity at some time, t, of this radionucleide, given the activity at t -equal, zero and the activity at some other time.
00:26
And so we can first realize what we were given.
00:30
The activity at the time t equals zero was 548 decays per second, and that decays per second is the unit of beccarell.
00:37
So this is 548 becorels.
00:40
We're also given the activity at the time t equals 48 minutes, which is 213 becorels.
00:47
And we can use this to find first to half -life.
00:50
If we, well, we can first write down the activity at any time t.
00:55
This is given as the activity at the time t equals 0 times e to the negative lambda t.
01:00
That's how it's typically written.
01:03
But we know that lambda is equal to the natural log of 2 over t 1 half based on the typical definition of the half life.
01:14
If you rearrange that just a little bit.
01:16
And if you plug that into this equation, this will be a sub 0, e to the negative natural log of 2 times t.
01:23
Over t one half and now we can solve for t one half and if we do that we will divide both sides by a sub zero and take the natural log so we'll have the natural log of a of t over a sub zero is equal to the negative natural log of two times t over t one half because the natural log of e to the x is just x so this right size we'll just become the exponent.
01:57
So now we can just solve for t one half if we multiply t one half on both sides and divide by this on both sides.
02:07
So we'll get that t one half is equal to the negative natural log of two times t over the natural log of a of t over a 0, which is relatively complicated at first.
02:23
But this allows us to calculate the half -life at any time.
02:25
Time t if we know the activity at that time.
02:29
And we were given that at time 48 minutes, we were given the activity...