Synchrotron radiation exhibits a wide spectrum due to the continuous range of energies that free electrons can achieve when accelerated in strong magnetic fields. While individual photons have specific energy values, the electrons can possess a continuum of energy states, especially when unbound by nearby charges. This continuous energy variation allows for the emission of photons across a broad spectrum, akin to conventional x-rays. The initial and final states of electrons in synchrotron accelerators are not quantized, leading to a continuous x-ray spectrum. Understanding this phenomenon requires a grasp of both classical and quantum theories of electron behavior.