LEVELJEE Main
Visualized Solution
The Sigma Insight: Nucleus and Nuclear Reaction
The phenomenon of nuclear disintegration is a fascinating display of fundamental physics principles in action. When a heavy parent nucleus at rest suddenly splits into two fragments, it sets the stage for a perfect application of the Law of Conservation of Linear Momentum.
Analyzing the Setup Imagine a parent nucleus sitting perfectly still
Its initial velocity is zero, which means its initial momentum is also zero. Suddenly, it disintegrates into two parts. Because there are no external forces acting on the system, the total momentum must remain conserved.
This implies that the two new fragments must fly apart in exactly opposite directions, and their momenta must be equal in magnitude. Mathematically, we express this as:
The Velocity-Mass Relationship The problem states that the velocities of the two fragments are in the ratio
Let's call the faster fragment part 1 and the slower one part 2. So, we have:
Using our momentum conservation equation, we can rearrange it to find the ratio of their masses:
Substituting the given velocity ratio, we get:
This tells us a crucial physical truth: the fragment that moves twice as fast must be half as massive. The lighter fragment is always the faster one!
Connecting Mass to Nuclear Size Now, we need to find the ratio of their nuclear sizes, which means the ratio of their radii
How do we connect mass to radius?
The key lies in the properties of nuclear matter. The density of nuclear matter, denoted by , is incredibly high but, more importantly, it is constant for almost all nuclei. Since density is mass per unit volume, we can write the mass of a spherical nucleus as:
Because and are constants, we can conclude that the mass of a nucleus is directly proportional to the cube of its radius:
Final Calculation
We can now substitute this proportionality into our mass ratio equation:
Since we already know that , we can equate the two:
To find the ratio of the radii, we simply take the cube root of both sides:
Therefore, the ratio of their nuclear sizes is:
This elegant result perfectly matches option (d). It's a beautiful reminder of how macroscopic conservation laws and microscopic nuclear properties intertwine to give us precise predictions about the subatomic world.
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