High School

On August 6th, 1945, the United States of America dropped a nuclear bomb on Hiroshima, Japan. Known as the "Little Boy," the nuclear device had a 2-part core that ultimately contained 64 kg of Uranium-235, which has a half-life of 700 million years.

Based on this, how many atoms of Uranium-235 would still be undergoing radioactive decay today?

Answer :

Final answer:

Using the half-life of Uranium-235, nearly all of the original 64 kg remains today, as its half-life is 700 million years compared to the 78 years since the bomb was dropped. Therefore, approximately 1.64 x 10²⁵ atoms of U-235 are still present. This demonstrates the stability and longevity of radioactive isotopes.


Explanation:

Calculating Remaining Atoms of Uranium-235

To determine how many atoms of Uranium-235 (U-235) remain today from the original 64 kg used in the Little Boy bomb dropped on Hiroshima, we can use the concept of half-life and the following formula:

Formula

N = N₀ (1/2)^(t/T_half)

  • N = number of atoms remaining
  • N₀ = initial number of atoms
  • t = time elapsed
  • T_half = half-life of U-235

First, we need to calculate the initial number of U-235 atoms:

1. Convert mass to moles:

Using the molar mass of U-235, which is approximately 235 g/mol:

64 kg = 64000 g

Number of moles (n) = mass/molar mass = 64000 g / 235 g/mol ≈ 272.34 moles.

2. Calculate number of atoms:

Using Avogadro's number (approximately 6.022 x 10²³ atoms/mol):

Number of atoms (N₀) = n × Avogadro's number = 272.34 moles × 6.022 x 10²³ atoms/mol ≈ 1.64 x 10²⁵ atoms.

3. Time elapsed since August 6, 1945:

As of today (let's assume it's October 2023), the time elapsed is:

2023 - 1945 = 78 years.

4. Convert years to years (since the half-life is already in years):

T_half = 700 million years.

5. Calculate remaining atoms:

N = N₀ (1/2)^(t/T_half)

N = 1.64 x 10²⁵ * (1/2)^(78/700000000) ≈ 1.64 x 10²⁵.

This indicates that nearly all of the original U-235 atoms would still be present and undergoing radioactive decay today due to the extremely long half-life relative to the time elapsed since the bomb's detonation.


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