Category Archives: Gravity

True Gravity and The Blueprint of The Universe: The Proof of

Dean E. Walker

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Measurements of the results are taken using a ruler and protractor. (Scale: 1 unit = 0.5 m ) (a) A + B = 5.2 m at 60° (b) A – B = 3.0 m at 330° (c) B – A = 3.0 m at 150° (d) A – 2B = 5.2 m at 300°. Virtual strings are the answers to almost all our questions about how physics works. R Once the coil is entirely inside the field, Φ B = NBA = constant, ε =0, I =0, so and F= 0. Atmanspacher and colleagues developed a detailed model predicting a quantitative relation between basic psychophysical time scales in bistable perception that has been confirmed experimentally (Atmanspacher and Filk 2013).

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Light in Einstein's Universe: The Role of Energy in

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Also derived from New Electromagnetism: Schwarzschild radius, E = m c2 is constant to all observers in all reference frames. If we take the bead to be perfectly absorbing, the light pressure is P = av = = c c A (a) F = Fg so I= F c Fg c mgc = =. The second reason gravity remained hidden for so long is that it is tremendously weak. No wonder they didn't bother to consult a physicist. But, the presentation (by the YouTuber) is nicely done, and it will be interesting to see how this information develops, in months and years ahead.

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The Relativistic Boltzmann Equation: Theory and Applications

Carlo Cercignani

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Like Newton's first law of motion, Einstein's theory states that if a force is applied on an object, it would deviate from a geodesic. The approximation assumes ∆w∆ ≈ 0, or α∆T ≈ 0. At t = 0, Φ B = π ar 2. a ε=− (c) I= (d) P31.60 P =εI= − ε=− π br 2 ε = − R R F GH a f d a + bt dΦ B = −π r 2 = −π br 2 dt dt (b) f π br 2 R I e−π br j = JK 2 π 2b 2r 4 R FG IJ H K d dB NBA = −1 π a2 = π a2K dt dt (a) Q = Cε = Cπ a 2 K (b) B into the paper is decreasing; therefore, current will attempt to counteract this.

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Naked Singularitium. Planck-Scale Partially Cloaked Black

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A massive tornado is hot on your tail and all you've got on your side is your old trusty bike. Magic, Inc. 1978, 1985, 1991. [MG-1] Illustrations from this book have been used below, with Mr. Chapter 32 241 Q32.14 When the capacitor is fully discharged, the current in the circuit is a maximum. Q26.17 The dielectric strength is a measure of the potential difference per unit length that a dielectric can withstand without having individual molecules ionized, leaving in its wake a conducting path from plate to plate.

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O Love! O Fire!

Denise Robins

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Which of the following To eight significant figures, Avogadro's constant is choices demonstrates correct rounding? Qc Therefore, ∆t ∆m = ∆t and P22.61 (a) = FG ∆m IJ c∆T = P T H ∆t K T − T c h c P Tc Th − Tc c∆T b g a f a f 5 98.6° F = a98.6 − 32.0f° C = a37.0 + 273.15f K = 310.15 K 9 dQ dT F 310.15 IJ = 54.86 cal K ∆S =z = b 453.6 g gb1.00 cal g ⋅ K g × z = 453.6 lnG H 274.82 K T T Q a310.15 − 274.82f = −51.67 cal K ∆S =− = −a 453.6 fa1.00f 35.0° F = 5 35.0 − 32.0 ° C = 1.67 + 273.15 K = 274.82 K 9 310.15 ice water 274.82 body Tbody 310.15 ∆Ssystem = 54.86 − 51.67 = 3.19 cal K (b) a453.6fa1fbT F g e ja fb − 274.82 = 70.0 × 10 3 1 310.15 − TF g Thus, b70.0 + 0.453 6g × 10 T = a70.0fa310.15f + b0.453 6ga274.82f × 10 3 F 3 and TF = 309.92 K = 36.77° C = 98.19° F FG 309.92 IJ = 54.52 cal K H 274.82 K F 310.15 IJ = −51.93 cal K = −e70.0 × 10 j lnG H 309.92 K ∆Sice water = 453.6 ln ′ ∆S body ′ 3 ∆Ssys = 54.52 − 51.93 = 2.59 cal K which is less than the estimate in part (a). ′ 655 656 P22.62 Heat Engines, Entropy, and the Second Law of Thermodynamics (a) For the isothermal process AB, the work on the gas is W AB = − PA VA ln FG V IJ HV K B A e 50 0 j FGH 10..0 IJK je W AB = −5 1.013 × 10 5 Pa 10.0 × 10 −3 m3 ln W AB = −8.15 × 10 3 J where we have used 1.00 atm = 1.013 × 10 5 Pa 1.00 L = 1.00 × 10 −3 m 3 and ja e FIG.

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Introduction to Conformal Field Theory: With Applications to

Erik Plauschinn

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So if something happens for the first time, it can't happen because it never happened before? Then the equivalent capacitance can be determined from the following circuit: ⇒ ⇒ FIG. Being on the slopes of Rattlesnake Mountain, a 3630 foot elevation treeless basalt mountain, it is in a region of unusually low microseismic background noise. in Proceedings of the 12th Marcel Grossmann Meeting on General Relativity , Paris 2009.

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Recent Advances in General Relativity (Einstein Studies)

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P23.50 Possible only with +51.3 µ C at x = −16.0 cm P23.12 md 3 where m is the mass k e qQ π (a) period = 2 k e qQ of the object with charge −Q; (b) 4a md 3 P23.14 1.49 g P23.16 720 kN C down P23.52 (a) 24.2 N C at 0°; (b) 9. 42 N C at 117° P23.18 (a) 18.0 i − 218 j kN C; P23.54 5.25 µC P23.56 (a) P23.58 0.205 µC e j (b) 36.0 i − 436 j mN mg mgA; (b) A cot θ + B A cos θ + B sin θ P23.20 (a) 12.9 j kN C; (b) −38.6 j mN P23.22 see the solution P23.24 π 2 ke q − i 6a2 P23.62 443 i kN C P23.26 keλ 0 −i x0 P23.64 0.072 9 a P23.28 keλ 0 −i 2x0 P23.66 see the solution; the period is P23.68 R P23.30 P23.32 P23.34 P23.60 e j e j (a) 383 MN C away; (b) 324 MN C away; (c) 80.7 MN C away; (d) 6.68 MN C away LMe j − ead + hf + R j N 2 k Qi L (b) R h M Nh + ed + R j − ead + hf + R j k eQ i d 2 + R2 h e 2 2 a2 toward the 29th vertex F mg I GH k 3 JK 12 e see the solution (a) k e qQ −1 2 2 12 2 2 2 −1 2 2 OP; Q OP Q 12 P23.70 (a) see the solution; (b) k P23.72 e−1.36i + 1.96 jj kN C π 81 4 mL3 k eQq 24 Gauss’s Law CHAPTER OUTLINE 24.1 24.2 24.3 Electric Flux Gauss’s Law Application of Gauss’s Law to Various Charge Distributions Conductors in Electrostatic Equilibrium Formal Derivation of Gauss‘s Law ANSWERS TO QUESTIONS 24.5 The luminous flux on a given area is less when the sun is low in the sky, because the angle between the rays of the sun and the local area vector, dA, is greater than zero.

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GRAVITATION: OUR QUANTUM TREASURE

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A new answer to this question and some commentary on the old answer. 6pp. 361. The proton is not even elementary but composed of quarks. Unfortunately, because the water is almost incompressible, this will be much deeper than the crush depth of the submarine. For example, the Moon’s centre of mass is very close to its geometric centre (it is not exact because the Moon is not a perfect uniform sphere), but its centre of gravity is slightly displaced toward Earth because of the stronger gravitational force on the Moon’s near side.

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Relativity, Gravitation and Cosmology: A Basic Introduction

Ta-Pei Cheng

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We divide this equation 3 3 for the larger sphere by the same equation for the smaller: For either sphere the volume is V = ρ 4π r 3 3 r 3 m = = = 5. m s ρ 4π rs3 3 rs3 a f Then r = rs 3 5 = 4.50 cm 1.71 = 7.69 cm. Fill several balloons with different gases such as air, carbon dioxide, natural gas, helium, and propane to about the same pressure. Typically, we are taught about the three states of matter; namely, solid, liquid, and gas. Friction exerts a force in the direction opposite to the direction in which something is moving or trying to move.

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Einstein's Field Equations and Their Physical Implications:

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For α > 0, γ is negative and multiple reflections from each mirror will occur before the incident and reflected rays intersect. 327 Chapter 35 Section 35.6 *P35.28 Huygen’s Principle (a) For the diagrams of contour lines and wave fronts and rays, see Figures (a) and (b) below. As more energy E is fed into the object E without limit, its speed approaches the speed of light and its momentum approaches. c Q39.13 Recall that when a spring of force constant k is compressed or stretched from its relaxed position a 1 distance x, it stores elastic potential energy U = kx 2.

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