Answer:
A. x = -㏑(1/2)/μ B. x = -㏑(I/I₀)/μ
Step-by-step explanation:
A. Since the intensity I = I₀exp(-μx) where I₀ = intensity at x = 0.
When I = I₀/2,
I = I₀exp(-μx)
I₀/2 = I₀exp(-μx)
dividing through by I₀, we have
1/2 = exp(-μx)
taking natural logarithm of both sides, we have
㏑(1/2) = ㏑[exp(-μx)]
㏑(1/2) = -μx
dividing both sides by -μ
x = -㏑(1/2)/μ
where x is the thickness of the material that would absorb half of the gamma rays
B. Since the intensity I = I₀exp(-μx) at thickness x, where I₀ = intensity at x = 0
I = I₀exp(-μx)
dividing through by I₀
I/I₀ = exp(-μx)
taking natural logarithm of both sides, we have
㏑(I/I₀) = ㏑exp(-μx)
㏑(I/I₀) = -μx
dividing both sides by -μ
x = -㏑(I/I₀)/μ
where x is the thickness of the material that would reduce the radiation intensity to a fraction of the initial intensity.