The study of radioactive decay often involves exponential functions, which can be tricky to analyze visually. However, by applying a simple mathematical transformation—the natural logarithm—we can turn a curved exponential graph into a straight line. This makes extracting crucial physical constants, like the half-life, incredibly straightforward. Let's dive into how this works!
Decoding the Graph
We are given a graph plotted with the natural logarithm of the decay rate (
lnR) on the y-axis and time (
t) on the x-axis. To understand what this line represents, we must start with the fundamental law of radioactive decay:
R=R0e−λt
where
R is the decay rate at time
t,
R0 is the initial decay rate, and
λ is the decay constant.
To match our graph, we take the natural logarithm on both sides of the equation:
lnR=ln(R0e−λt)
Using the properties of logarithms, this simplifies to:
lnR=−λt+lnR0
Extracting the Physics
Notice the beautiful structure of this new equation. It perfectly mirrors the standard equation of a straight line, y=mx+c.
Here, our y-variable is lnR, our x-variable is t, the y-intercept c is lnR0, and most importantly, the slope m is exactly −λ.
This means that if we can find the slope of the line from the graph, we immediately know the decay constant! Let's pick two easy-to-read points from the graph:
1. The y-intercept: At t=0, lnR=6. So, (t1,y1)=(0,6).
2. The x-intercept: At t=40 s, lnR=0. So, (t2,y2)=(40,0).
Now, we calculate the slope
m:
m=t2−t1y2−y1=40−00−6=−406
Since we established that
m=−λ, we have:
−λ=−406⟹λ=406=0.15 s−1
The Final Calculation
The question asks for the half-life (
t1/2) of the material. The half-life is inversely proportional to the decay constant, given by the formula:
t1/2=λln2≈λ0.693
Substituting our exact fractional value for
λ to avoid early rounding errors:
t1/2=(406)0.693=60.693×40
Performing the final arithmetic:
t1/2=0.1155×40=4.62 s
The half-life of the unknown radioactive material is approximately 4.62 seconds.
By simply understanding the geometry of the graph, we unlocked the hidden physics of the radioactive sample!