- #1
artis
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So I see EM radiation , visible spectrum including being portrayed as two sinewave vectors each perpendicular to other one being that of the E field the other being the B field, the field is carried by photons, let's take the visible spectrum as an example.
So having a specific frequency the radiation has a specific wavelength , another property from frequency is the energy that each individual photon carries at that frequency.
Here is my question, how can each photon carry the same energy at any given frequency if a sinewave has peaks and then closer to the so called "zero crossing" it has very little energy if any?
Or am I confusing this with how electrons move in a wire in the case of AC when at peaks they have their maximum potential while near midpoint they have almost no energy? Does this only work for currents and charged particles with mass and isn't applicable to massless photons ?
So having a specific frequency the radiation has a specific wavelength , another property from frequency is the energy that each individual photon carries at that frequency.
Here is my question, how can each photon carry the same energy at any given frequency if a sinewave has peaks and then closer to the so called "zero crossing" it has very little energy if any?
Or am I confusing this with how electrons move in a wire in the case of AC when at peaks they have their maximum potential while near midpoint they have almost no energy? Does this only work for currents and charged particles with mass and isn't applicable to massless photons ?