In relativistic physics, the Lorentz factor \( \gamma \) plays a crucial role in understanding how time, length, and energy transform when an object approaches the speed of light. It is defined by the formula \( \gamma = \frac{1}{\sqrt{1-(v/c)^2}} \), where \( v \) is the object's speed, and \( c \) is the speed of light.
As the speed \( v \) of an object gets closer to the speed of light \( c \), the Lorentz factor \( \gamma \) increases significantly. This implies that at very high speeds, even small increases in speed require large amounts of energy, impacting how we calculate kinetic and total energy.
- When \( v = 0 \), \( \gamma = 1 \)
- As \( v \to c \), \( \gamma \to \infty \)
These transformations explain why classical mechanics doesn't hold at high velocities and highlight the need for relativistic physics.