A common example of alpha decay is

Energy released \( Q \) is given by the equation: \[ Q = (\Delta m)_{\text{amu}} \times 931.5 \, \text{MeV}. \] Here, the mass defect \( \Delta m \) is: \[ \Delta m = m_u - m_{\text{Th}} - m_{\text{He}} = 238.05060 \, u - 234.04360 \, u - 4.00260 \, u = 0.0044 \, u. \] Thus, \[ Q = 0.0044 \times 931.5 \, \text{MeV} = 4.0986 \, \text{MeV}. \] Therefore, the energy released during the alpha decay of \( ^{238}_{92} U \) is 4.0986 MeV.
A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)): 
0.01 mole of an organic compound (X) containing 10% hydrogen, on complete combustion, produced 0.9 g H₂O. Molar mass of (X) is ___________g mol\(^{-1}\).
If the system of equations \[ (\lambda - 1)x + (\lambda - 4)y + \lambda z = 5 \] \[ \lambda x + (\lambda - 1)y + (\lambda - 4)z = 7 \] \[ (\lambda + 1)x + (\lambda + 2)y - (\lambda + 2)z = 9 \] has infinitely many solutions, then \( \lambda^2 + \lambda \) is equal to: