Step 1: Effect of Alpha ( \( \alpha \) ) Decay
An alpha particle (\( \alpha \)) has a mass number of 4 and an atomic number of 2.
When element \( X \) undergoes alpha decay:
$$ {^{290}_{82}X -> ^{286}_{80}Y + ^{4}_{2}\alpha} $$
Thus, the new nucleus \( Y \) has:
Mass number = \( 290 - 4 = 286 \)
Atomic number = \( 82 - 2 = 80 \)
Step 2: Effect of Positron (\( e^+ \)) Emission
Positron emission (\( \beta^+ \)) decreases the atomic number by 1 without changing the mass number:
$$ {^{286}_{80}Y -> ^{286}_{79}Z + e^+} $$
Thus, \( Z \) has:
Mass number = 286 (unchanged)
Atomic number = \( 80 - 1 = 79 \)
Step 3: Effect of Beta-Minus (\( \beta^- \)) Decay
Beta-minus (\( \beta^- \)) emission increases the atomic number by 1 without affecting the mass number:
$$ {^{286}_{79}Z -> ^{286}_{80}P + \beta^-} $$
Thus, \( P \) has:
Mass number = 286 (unchanged)
Atomic number = \( 79 + 1 = 80 \)
Step 4: Effect of Electron Capture (\( e^- \))
Electron capture decreases the atomic number by 1, keeping the mass number unchanged:
$$ {^{286}_{80}P + e^- -> ^{286}_{81}Q} $$
Thus, \( Q \) has:
Mass number = 286 (unchanged)
Atomic number = \( 80 + 1 = 81 \)
Conclusion
The final product \( Q \) has mass number 286 and atomic number 81, which corresponds to option (4).
Mass Defect and Energy Released in the Fission of \( ^{235}_{92}\text{U} \)
When a neutron collides with \( ^{235}_{92}\text{U} \), the nucleus gives \( ^{140}_{54}\text{Xe} \) and \( ^{94}_{38}\text{Sr} \) as fission products, and two neutrons are ejected. Calculate the mass defect and the energy released (in MeV) in the process.
Given:
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The current passing through the battery in the given circuit, is:
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