« Reply #13 on: October 04, 2022, 02:50:40 AM »
close local light source, if you've seen a street light when it's a foggy night, you see the divergent/cerpuscular rays, similar to the rays we ovserve from the sun, without assuming or presuming a distant sun and the refraction that would be required. The last picture is where the camera is held up to eye level, all the other ones are siting on the ground and moving away from the 2 lids, on a flat warehouse floor. So the last two photos are the same distance but the last one he brings the camera up, increasing the angle, and you can then make out what was being obscured by the defraction at the horizon. Now these optics work in conjunction with the optics from the video with rob skiba, showing that with enough moisture in the air we can see how objects can apear to be magnified, and sink below the horizon, and the defraction demonstrates why it may be assumed things disappear from the bottom up, even on a flat surface. I hope that was concise enough. I might be able to link the video these photos were pulled from if you want to hear it explained in a different way.
Do you have rokfin? Chicago skyline experiment 1 @ -151 I'll find the defraction explanation wren i find it.
https://rokfin.com/stream/20360
i found it. If you don't have rokfin, you can probably find them through odyssey/lbry.
It's around @ -105
https://rokfin.com/stream/21248
3 16:38
➽ I just want to recap, we agree what we observe is a close local light source, and the notion of a distant sun requires presumptions, correct?
Yes... With caveat... The (my) alleged proof of a distant sun has NOT been verified, thus the (my) alleged proof is just a presumption until verified.
In my 30 14:54 post I said:
My sole point is the angle to the top of a structure is measurable and different according to the two models/theories.
The image attached, created for discussion with another, shows the fact that the closer one is to an object, the higher the angle to the top will be. Close enough and atmospheric issues are not observable. However close enough to see 1° GE-FE difference is far enough away to be affected by the atmosphere.
1.0 nautical mile = 1.150779 mile = 1/60 of a degree = 1 minute
So one degree = 69. nautical miles = 79.5 statute miles.
My image is 49.5 miles.
According to the curve calculator, the top of an object must be taller than 3,915 feet to be observed over the (assumed) curvature to verify a 1 degree difference due to roundness.
Your part in this discussion has caused me to conclude my image is NOT suitable as proof of GE. Likewise, the images you presented of Chicago are NOT suitable as proof of FE. Score one for you, personally. Adds nothing to the FE score though.
In my 3 15:22 post I quoted Wiki:
⚡Whenever possible, astronomers will schedule their observations around the times of culmination, when celestial objects are highest in the sky. Likewise, sailors will not shoot a star below 20° above the horizon.⚡
The errors caused by atmosphere are known and accounted for in celestial navigation. I did not know such errors would be so pronounced until looking into the optics of atmosphere due to this convo.
Now my curiosity is going to demand I visit that beach several times during the year. My A Priori theory is that I will see differing amounts of occlusion.
The attached image also shows the farther away the item observed, the smaller its angular size will be.
Angular size in degrees = inverse-tangent(size ÷ distance)
Distance = size ÷ tangent(angle)
Size = distance × tangent(angle)
The angular size of both the sun and the moon are about .5°
.5° = Inverse-tangent(0.0087268677907587893345361980612)
Distance to the sun = sun's size ÷ 0.00872
Sun's size = sun's distance × 0.00872
Distance to the moon = moon's size ÷ 0.00872
Moon's size = moon's distance ÷ 0.00872
My notes for the record and future point reminder:
The moon's angular size equals the sun's angular size because of total eclipse.
The moon is closer to earth than the sun because of total eclipse.
Moon - sun distance ratio and moon - sun size ratio will be the same.
Double distance:double size, 3X:3X, 4X:4X, etc.
« Last Edit: October 04, 2022, 02:40:05 PM by Dale Eastman »
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