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Question 10
Read the following passage and answer the accompanying questions. Ernest Walton was one of the legendary pioneers who made 1932 the annus mirabilis of experimental ... show full transcript
Step 1
Answer
To illustrate how Cockcroft and Walton accelerated protons, we can depict the following components:
This diagram should label each part and show the direction of the proton beam towards the lithium target.
Step 2
Answer
The kinetic energy gained by the proton when accelerated through a potential difference is given by the equation:
Where:
Plugging in the values:
The kinetic energy can also be expressed as:
Thus,
Where is the mass of the proton = . Therefore:
Step 3
Answer
The nuclear equation for the disintegration of a lithium-6 nucleus when bombarded with a proton can be written as follows:
In this reaction:
Step 4
Answer
To calculate the energy released, we need to find the mass defect and convert it to energy using Einstein's equation:
The masses involved are:
The mass before the reaction (reactants):
The mass after the reaction (products):
Then, the mass defect is:
Now we convert this mass defect to energy:
Calculating:
Step 5
Answer
Electrons and positrons share several properties but also have key differences:
In summary, while they possess equal mass and spin, the critical difference lies in their electric charge.
Step 6
Answer
When an electron meets a positron, they can annihilate each other, resulting in the production of gamma-ray photons. This annihilation process typically results in the release of two photons, each carrying energy corresponding to the mass of the electron and positron, and can be described by the equation: where is the mass of the electron (or positron). This process conserves energy and momentum.
Step 7
Answer
Fermi's theory of radioactive decay proposed that during beta decay, a neutron decays into a proton, an electron, and an antineutrino. The inclusion of the antineutrino provided a mechanism for conserving both energy and momentum in the decay process. The antineutrino carries away any excess momentum, ensuring that the overall conservation laws are upheld. This was a significant advancement in understanding weak interactions and decay processes in particle physics.
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