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In any fission process the ratio

 mass of fission products  mass of parent nucleus  is:

1. Greater than 1

2. Depends on the mass of the parent nucleus

3. Equal to 1

4. Less than 1

Subtopic:  Nuclear Energy |
 61%
Level 2: 60%+
AIPMT - 2005
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Fission of nuclei is possible because the binding energy per nucleon in them:
 

1. decreases with the mass number at low mass numbers
2. increases with the mass number at low mass numbers
3. decreases with the mass number at high mass numbers
4. increases with the mass number at high mass numbers
Subtopic:  Nuclear Energy |
 61%
Level 2: 60%+
AIPMT - 2005
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Nuclear–fission is best explained by:
1. Liquid droplet theory.
2. Yukawa \(\pi\text-\)meson theory.
3. Independent particle model of the nucleus.
4. Proton-proton cycle.
Subtopic:  Nuclear Energy |
Level 3: 35%-60%
AIPMT - 2000
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For the nuclear reaction:
\({}_{92}^{235}\mathrm{U}+ {}_{0}^{1}\mathrm{n}\rightarrow {}_{56}^{144}\mathrm{Ba}+...+3{}_{0}^{1}\mathrm{n}\)
The blank space can be filled by:
1. \({}_{26}^{89}\mathrm{Kr}\) 2. \({}_{36}^{89}\mathrm{Kr}\)
3. \({}_{26}^{90}\mathrm{Sr}\) 4. \({}_{38}^{89}\mathrm{Sr}\)
Subtopic:  Nuclear Energy |
 89%
Level 1: 80%+
AIPMT - 1998
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Xmn emitted one αand2β particles, then it will become: 

1. Xm-4n

2. Xm-1n-1

3. Zm-4n

4. None of these

Subtopic:  Types of Decay |
 72%
Level 2: 60%+
AIPMT - 1998
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When \(\mathrm{X}\rightarrow {}_{7}^{14}\mathrm{N}+2\beta^{-}\) then the number of neutrons in \(\mathrm{X}\) will be:
1. \(3\)
2. \(5\)
3. \(7\)
4. \(9\)

Subtopic:  Types of Decay |
 61%
Level 2: 60%+
AIPMT - 1998
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If in a nuclear fusion process. the masses of the fusing nuclei be \(m_1\) and \(m_2\) and the mass of the resultant nucleus be \(m_3,\) then:
1. \( m_3=\left|m_1-m_2 \right|\) 2. \( m_3<\left ( m_1+m_2 \right ) \)
3. \( m_3>\left ( m_1+m_2 \right ) \) 4. \( m_3=\left ( m_1+m_2 \right ) \)
Subtopic:  Nuclear Binding Energy |
 80%
Level 1: 80%+
AIPMT - 2004
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A nucleus represented by the symbol \({}_{Z}^{A}\mathrm{X}\) has:
1. \(Z\) protons and \(A-Z\) neutrons
2. \(Z\) protons and \(A\) neutrons
3. \(A\) protons and \(Z-A\) neutrons
4. \(Z\) neutrons and \(A-Z\) protons
Subtopic:  Nuclear Binding Energy |
 91%
Level 1: 80%+
AIPMT - 2004
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\(M_p\) denotes the mass of a proton and \(M_n\) that of a neutron. A given nucleus, of binding energy \(B\), contains \(Z\) protons and \(N\) neutrons. The mass \(M(N,Z)\) of the nucleus is given by:
(\(c\) is the velocity of light )
1. \(M(N,Z)= NM_n+ZM_p+ Bc^2\)
2. \(M(N,Z)= NM_n+ZM_p-\frac{B}{c^2}\)
3. \(M(N,Z)= NM_n+ZM_p+\frac{B}{c^2}\)
4. \(M(N,Z)= NM_n+ZM_p- Bc^2\)

Subtopic:  Nuclear Binding Energy |
 87%
Level 1: 80%+
AIPMT - 2004
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If a radioactive element emitted one \(\alpha\) and one \(\beta\text-\)particle, then the mass number of the daughter element is:
1. decreased by \(4\)
2. increased by \(4\)
3. decreased by \(2\)
4. increased by \(2\)

Subtopic:  Types of Decay |
 88%
Level 1: 80%+
AIPMT - 1999
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