Moon, BLACK BODY RADIATION AND absurdities of modern physicsLong ago I proposed a variation on the phases of experiment and how this phenomenon contradicts the quantum hypothesis, since the emission maximum should change in infrared oven according to the received illumination from the sun. The experiment was published in the book on the corpuscular nature of light, but when it was thought , the Internet was something that was reduced to a simple exchange of emails.Now I am working on a new theory of thermodynamics and book reference of Astronomy and Astrophysics ,so it is time to revisit the subject and possibly compare with what theory implies measured experimentally.So, the Moon, Earth's Moon has a radius of about 1750 km, and its surface temperature is ranging from 105 C to -170 C. sunny face face shaded Recall that established the following law Planck energy distribution in the spectrum of thermal radiation:

Figure 1. Spectral distribution formula proposed by PlanckTheorists thought that Planck's hypothesis and proposed distribution of it (Fig. 1), is modeled quite well with the spectral distribution emitted by a series of heavenly bodies (sun, moon, etc).Planck's law allows us to calculate how much energy is emitted per unit area of a black body at a certain temperature. As initial measurements were made in the infrared energy emitted constants and expression has been adapted to this area. In the calculations that follow, the discussion extends from the infrared to the microwave and radio frequency energy and at the same time a conversion is made of the results of IR-specific expression of the specific radio area.Calculating how much is emitted by unit area at a specific wavelength radio and then summing over the entire surface emissivity value shaded can find out how much the Moon surface emits a specific wavelength.For example, 4 mm, or 4000 m (in the oven), the shaded area, we have that specific emissivity of the month, according to Planck distribution is:In this wavelength Luna would emit power:

Expression emissivity as W / m2m that is not suitable for the radio and therefore must move to a form of expression of W / m2Hz or W / Hz. To this end, one can not directly convert the frequency wavelengths sizes are differentiated as Planck's formula and must use the following conversion formula: If we do the calculations for 4mm that the moon emits per unit area about: If emission per unit area at the level of EL- is then in the Earth's orbit reaches the surface per unit EP- can be calculated with the formula:

where LPL = 385000 km and RL = 1750 km. Substituting we have:

Considering only the shaded part , at 100K, it should emit electromagnetic waves in the microwave, radio and IR, and in Table 1 are calculated for several wavelengths of emissivity values of these fields, and the stream reach on Earth.

Nr. crt.wavelengthPower output per unit. surface. wavelength W/m2mEmissive power of the wavelength W/mPower output per unit. surface. frequencyW/m2HzEmissive power of the frequency W/HzThe flow of the unit. surface. that can be measured on Earth at frequency W/m2Hz

Field emission optical IR, VIS, UV

110m2.11E-034.07E+047.05E-221.36E-141.46E-26

225m1.22E-012.34E+062.54E-194.88E-125.24E-24

350m7.14E-021.37E+065.95E-191.14E-111.23E-23

475m2.72E-025.22E+055.09E-199.79E-121.05E-23

5100m1.16E-022.24E+053.88E-197.46E-128.02E-24

6200m1.11E-032.14E+041.48E-192.85E-123.06E-24

7300m2.50E-044.81E+037.51E-201.44E-121.55E-24

8400m8.44E-051.62E+034.50E-208.66E-139.31E-25

9500m3.59E-056.91E+022.99E-205.76E-136.19E-25

10600m1.78E-053.42E+022.13E-204.10E-134.40E-25

11700m9.76E-061.88E+021.59E-203.07E-133.29E-25

12800m5.80E-061.12E+021.24E-202.38E-132.56E-25

13900m3.66E-067.03E+019.87E-211.90E-132.04E-25

Field RADIO I MICROWAVES

MICROWAVES

141 mm2.42E-064.65E+018.06E-211.55E-131.67E-25

153 mm3.14E-086.03E-019.41E-221.81E-141.94E-26

164 mm9.98E-091.92E-015.32E-221.02E-141.10E-26

176 mm1.98E-093.81E-022.38E-224.58E-154.92E-27

188 mm6.29E-101.21E-021.34E-222.58E-152.77E-27

RADIO

191 cm2.58E-104.97E-038.61E-231.66E-151.78E-27

202 cm1.62E-113.12E-042.16E-234.15E-164.46E-28

213 cm3.20E-126.16E-059.61E-241.85E-161.99E-28

224 cm1.01E-121.95E-055.41E-241.04E-161.12E-28

235 cm4.16E-137.99E-063.46E-246.66E-177.16E-29

246 cm2.01E-133.86E-062.41E-244.63E-174.97E-29

257 cm1.08E-132.08E-061.77E-243.40E-173.65E-29

268 cm6.35E-141.22E-061.35E-242.60E-172.80E-29

279 cm3.96E-147.62E-071.07E-242.06E-172.21E-29

2810 cm2.60E-145.00E-078.67E-251.67E-171.79E-29

291,1 m1.78E-183.42E-117.17E-271.38E-191.48E-31

301,2 m1.25E-182.41E-116.02E-271.16E-191.24E-31

311,3 m9.11E-191.75E-115.13E-279.87E-201.06E-31

321,4 m6.77E-191.30E-114.42E-278.51E-209.14E-32

331,5 m5.14E-199.88E-123.85E-277.41E-207.96E-32

341,6 m3.97E-197.63E-123.39E-276.51E-207.00E-32

351,7 m3.11E-195.99E-123.00E-275.77E-206.20E-32

361,8 m2.48E-194.77E-122.68E-275.15E-205.53E-32

371,9 m2.00E-193.84E-122.40E-274.62E-204.96E-32

Tabelul1. Moon at 100 kAs shown, the flow value which should reach the Earth's surface is within reasonable limits for the current experimental technique. Thus the wavelength of 1.9M, the flow reaching the ground is of the order of 5Jy and as the wavelength decreases, the flow increases to be equal to 16,7Jy reached in the oven at 1 mm.If we calculate the values of sunny surface have values tab. February

Nr. crt.wavelengthPower output per unit. surface. wavelength W/m2mEmissive power of the wavelength W/mPower output per unit. surface. frequencyW/m2HzEmissive power of the frequency W/HzThe flow of the unit. surface. that can be measured on Earth at frequency W/m2Hz

Field emission optical IR, VIS, UV

110m1.05E+022.03E+153.52E-176.76E-047.27E-22

225m1.19E+012.29E+142.48E-174.78E-045.13E-22

350m1.14E+002.19E+139.48E-181.82E-041.96E-22

475m2.56E-014.93E+124.81E-189.24E-059.93E-23

5100m8.65E-021.66E+122.88E-185.54E-055.96E-23

6200m5.94E-031.14E+117.92E-191.52E-051.64E-23

7300m1.21E-032.33E+103.63E-196.98E-067.50E-24

8400m3.89E-047.47E+092.07E-193.99E-064.28E-24

9500m1.61E-043.09E+091.34E-192.57E-062.76E-24

10600m7.79E-051.50E+099.35E-201.80E-061.93E-24

11700m4.22E-058.12E+086.90E-201.33E-061.43E-24

12800m2.48E-054.78E+085.30E-201.02E-061.09E-24

13900m1.55E-052.99E+084.20E-208.07E-078.67E-25

Field RADIO I MICROWAVES

MICROWAVES

141 mm1.02E-051.97E+083.41E-206.55E-077.04E-25

153 mm1.28E-072.46E+063.83E-217.37E-087.92E-26

164 mm4.05E-087.78E+052.16E-214.15E-084.46E-26

176 mm8.01E-091.54E+059.61E-221.85E-081.98E-26

188 mm2.53E-094.88E+045.41E-221.04E-081.12E-26

RADIO

191 cm1.04E-092.00E+043.46E-226.66E-097.15E-27

202 cm6.50E-111.25E+038.66E-231.67E-091.79E-27

213 cm1.28E-112.47E+023.85E-237.41E-107.96E-28

224 cm4.06E-127.81E+012.17E-234.17E-104.48E-28

235 cm1.66E-123.20E+011.39E-232.67E-102.87E-28

246 cm8.03E-131.54E+019.63E-241.85E-101.99E-28

257 cm4.33E-138.33E+007.08E-241.36E-101.46E-28

268 cm2.54E-134.89E+005.42E-241.04E-101.12E-28

279 cm1.59E-133.05E+004.28E-248.23E-118.85E-29

2810 cm1.04E-132.00E+003.47E-246.67E-117.17E-29

291,1 m7.11E-181.37E-042.87E-265.51E-135.92E-31

301,2 m5.02E-189.65E-052.41E-264.63E-134.98E-31

311,3 m3.64E-187.01E-052.05E-263.95E-134.24E-31

321,4 m2.71E-185.21E-051.77E-263.40E-133.66E-31

331,5 m2.06E-183.95E-051.54E-262.97E-133.19E-31

341,6 m1.59E-183.05E-051.36E-262.61E-132.80E-31

351,7 m1.25E-182.40E-051.20E-262.31E-132.48E-31

361,8 m9.91E-191.91E-051.07E-262.06E-132.21E-31

371,9 m7.99E-191.54E-059.61E-271.85E-131.99E-31

From Table 2 shows that the amount of microwave and radio flux reaching the Earth blackbody formula predicted to be increasing. Thus the wavelength of 1.9M, the flow reaching the ground is of the order of 19 Jy and as the wavelength decreases, the flow increase, reaching 70.4 Jy equal to 1 mm in the microwave.But the surprise comes when we compare these data with what is measured experimentally for the moon. The information published in the literature (Fig. 2), the Moon has an emissivity in the microwave radio and much higher than could be explained by the theory of black body. Thus at a wavelength of 1.9 m month issue reaches approximately 10 Jy, and the 1mm becomes (by extrapolation) about 1,000,000 Jy.Such a deviation can not be attributed to experimental error. Basically radio astronomers know that after the Sun, the Moon appears to be the brightest object in the sky in the radio in our immediate vicinity.But how can the moon to issue such strength in radio?Current science is unable to provide a credible explanation at all!Figure 2. The spectrum of galactic and extragalactic radio sources (Kraus, 1986)From what I found in the internet is worth mentioning here a very interesting information. Illuminated surface becomes a source of radio waves and microwaves appreciable partially polarized after a certain time from the start of illumination by the sun. It's like the principle of old radios with lamp. It needed some time to warm lamps to have radio emission. Unfortunately, I do not know the moon to have such lamps in its composition. then how is it possible to convert a luminous flux month in a microwave radio stream?The theory is proposed, radio waves and light are completely different phenomena and none of them does not satisfy Maxwell's equations.The explanation of this phenomenon will be given in the following material which will be a summary of the differences between electromagnetic waves and photons. Of course you can organize a laboratory experiment to simulate conditions in the month and thus can verify the proposed explanation.