On The Study of Quantum Mechanics Behind the Bowcaster
Abstract:
The spreading of shots or 'slugs' can be quantised by observing the relationship between the wavelength of the 'slug', the distance from the barrel, and the slit separation, which is a set of 2 slits spaced at equidistance, similar to those used in Young's Double Slit Experiment. When the bow is charged, the slug released appear to exist in a single, shared space, at a given instance, and are concentrated, however, we know that no 2 matter can occupy the same space, and we can therefore surmise that the 'slugs', which we will now refer to as light, is a wave, rather than a particle that spreads up, or multiple particles that concentrate when the Bowcaster is charged. This would mean that the particles interact with each other as they pass through the barrel of the Bowcaster, which must contain a double slit. On the other hand, when the lights are released uncharged, it follows a predictable trajectory, and they space themselves out in a 102030201 pattern - where the number corresponds to the relative intensity, with fringe separation in between - almost as if they are interacting. They are therefore also a particle. This means the light excreted by the Bowcaster is in a wave-particle duality. We can measure the separation between each uncharged light pieces at a given distance with the given formula:
? = ax/D
rearranged to
x = ? * D /a
where ? is the wavelength of the light in its wave state, which, for green, is anywhere in the range of 492 and 577 nanometres, and we will use an arbitrary modal mean of
4.50 * 10^-9 meters.
'a' is the slit separation,
'x' is the fringe separation between the light bolts,
and 'D' is the distance of the light from the double slits.
We know the constant ? , but not the constant a, and must therefore experiment.
Abstract:
The spreading of shots or 'slugs' can be quantised by observing the relationship between the wavelength of the 'slug', the distance from the barrel, and the slit separation, which is a set of 2 slits spaced at equidistance, similar to those used in Young's Double Slit Experiment. When the bow is charged, the slug released appear to exist in a single, shared space, at a given instance, and are concentrated, however, we know that no 2 matter can occupy the same space, and we can therefore surmise that the 'slugs', which we will now refer to as light, is a wave, rather than a particle that spreads up, or multiple particles that concentrate when the Bowcaster is charged. This would mean that the particles interact with each other as they pass through the barrel of the Bowcaster, which must contain a double slit. On the other hand, when the lights are released uncharged, it follows a predictable trajectory, and they space themselves out in a 102030201 pattern - where the number corresponds to the relative intensity, with fringe separation in between - almost as if they are interacting. They are therefore also a particle. This means the light excreted by the Bowcaster is in a wave-particle duality. We can measure the separation between each uncharged light pieces at a given distance with the given formula:
? = ax/D
rearranged to
x = ? * D /a
where ? is the wavelength of the light in its wave state, which, for green, is anywhere in the range of 492 and 577 nanometres, and we will use an arbitrary modal mean of
4.50 * 10^-9 meters.
'a' is the slit separation,
'x' is the fringe separation between the light bolts,
and 'D' is the distance of the light from the double slits.
We know the constant ? , but not the constant a, and must therefore experiment.
