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 bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :