- Vector Model of Atom; Coupling of Orbital & Spin Angular Momentum
- Nuclear Parity & Pairing Energy
- Proportional Counter: Nuclear Radiation Detectors
- Particle Detectors: Nuclear Radiation Detectors
- Nuclear Fusion and Solar Energy
- Wilson Cloud Chamber (Principle, Construction & Working)
- Nuclear Reactions & Compound Nucleus Hypothesis
- Ionization Chamber: Nuclear Radiation Detectors
- Specific distribution in black body radiations
Here we discuss a mathematical interpretation of the Q values of nuclear reactions. In a nuclear reaction, not only the atomic number and mass number is conserved but also total energy remains conserved. Let us consider the nuclear reaction :
X + a ———> Y + b ……..(i)
Let Mx, Ma, My & Mb be the rest masses of X, a, Y and b respectively & Ea, Ey and Eb be the kinetic energy of a, Y and b respectively. The target nucleus X is initially at rest, so it has no kinetic energy.
By the conservation of total energy, the equation (i) can be written as :
Let Q be the energy released or absorbed during the nuclear reaction. It is the difference between the kinetic energy of the product of reaction & that of the initial interacting particle. i.e.
Reactions for which Q is positive called exothermic reaction & reactions for which Q is negative called endothermic reactions. This is how we have mathematically discussed Q values of nuclear reactions.