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maphth · 4 years
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maphth · 4 years
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Reminded me of Brownian motion
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maphth · 4 years
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The Japanese meteorological satellite, Himawara, captures the image of a Earth every 10min. This image is from last week.
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maphth · 6 years
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maphth · 6 years
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maphth · 6 years
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maphth · 6 years
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7149
7149! = 35 858 758 095 024 347 157 602 573 239 702 249 592 277 249 666 498 750 146 598 981 767 405 743 279 974 373 314 375 015 724 036 939 026 574 587 557 493 242 643 220 357 428 483 979 270 452 109 359 728 711 122 184 763 930 355 075 096 469 402 363 094 645 253 786 036 123 416 464 040 536 457 153 729 320 111 930 983 063 804 749 561 889 321 971 163 646 435 672 083 257 225 638 881 792 408 283 007 318 607 358 085 181 380 575 045 049 696 893 921 903 352 456 688 138 899 017 871 193 612 947 493 493 968 764 755 614 495 966 041 753 332 394 615 548 028 534 875 633 717 770 677 478 580 709 103 949 220 570 259 468 539 633 067 024 062 539 708 108 054 405 396 476 842 885 689 184 164 533 250 557 154 887 160 484 060 267 771 880 426 648 691 151 835 634 403 938 695 745 796 885 961 449 991 269 879 669 782 610 145 879 599 349 796 994 331 712 506 916 645 358 041 704 580 422 706 129 129 361 060 625 803 758 559 578 999 182 103 718 975 378 427 735 761 059 912 301 756 356 858 812 656 879 296 854 655 082 663 20
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maphth · 6 years
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maphth · 6 years
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maphth · 6 years
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From Stephen Hawking’s - Singularities and the Geometry of Spacetime, 2014
the Minkowski space
The cylinder represents R1 ×S3 where two spatial dimensions have been suppressed. The shaded region is the part conformal to Minkowski space.
This representation is a bit difficult to grasp as it is hard to visualise objects in four dimensions or to draw diagrams of them. However, it can be simplified using the fact that Minkowski space, as all the other solutions to be described, has spherical symmetry.
the Schwarzschild solution
The Penrose diagram of the t−r plane of Minkowski space. The dotted lines represent curves of constant r.
The Schwarzschild solution represents the spherically symmetric gravitational field outside some massive body. All the experiments which have been carried out to test differences between the general theory of relativity and Newtonian theory are based on predictions by this solution.
Eur. Phys. J. H DOI: 10.1140/epjh/e2014-50013-6
© EDP Sciences, Springer Verlag 2014
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maphth · 6 years
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Radial Triangles - 171004
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maphth · 6 years
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Diver
More of my work
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maphth · 6 years
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maphth · 6 years
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maphth · 6 years
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Spaceman
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maphth · 6 years
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Black holes aren’t black
They’re very dark, sure, but they aren’t black. They glow, slightly, giving off light across the whole spectrum, including visible light.
This radiation is called “Hawking radiation”, after the former Lucasian Professor of Mathematics at Cambridge University Stephen Hawking, who first proposed its existence. Because they are constantly giving this off, and therefore losing mass, black holes will eventually evaporate altogether if they don’t have another source of mass to sustain them; for example interstellar gas or light.
Smaller black holes are expected to emit radiation faster compared to their mass than larger ones, so if – as some theories predict – the Large Hadron Collider creates minuscule holes through particle collisions, they will evaporate almost immediately. Scientists would then be able to observe their decay through the radiation.
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maphth · 6 years
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Faraday’s Law of Electromagnetic Induction
The ball (also a magnet) is falling quite a bit slower than expected (despite the slow motion). This can be attributed to Faraday’s Law:
When a conductor is exposed to a changing magnetic field there is a current created within the conductor. Or more technically a magnetic flux changing over time produces an electromotive force across a conductor.
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That’s not the whole explanation though…
Lenz’s Law
When the magnet is falling the current in the cylinder is producing a magnetic field as well. Lenz’s Law states:
 The induced current will produce a new magnetic field that will oppose the change in magnetic flux.
The produced field applies a force to the magnet resisting its fall. If the tube is long enough the magnet will reach a constant velocity because the magnetic force and weight will cancel each other out (no net force).
This works like air resistance on a falling object. Eventually the resistance completely counters the gravitational acceleration of the object.
Faraday’s and Lenz’s Laws basically tell us that the faster the magnet moves the more the conductor (tube) will resist the magnet’s fall.
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Watch this Veritasium video on the same concept and see this phenomenon in real time.
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