Both ends of the S must be joint into a close loop becoming an infinite loop of the Hopf link. Incidentally, there are two loops locked together.
Both ends of the S must be joint into a close loop becoming an infinite loop of the Hopf link. Incidentally, there are two loops locked together.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Mobiusly speaking, it's a twisted infinite loop. This twist makes the Mobius surface one-sided.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
This is properly a local infinitesimal motion between each cycle of the topology, switching right and left, top and bottom, forward and backward.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
The swinging pendulum has another component of motion that demonstrate Earth's rotation around its axis. This is called the Foucault's pendulum. The one I saw is located at the Smithsonian Museum in Washington DC
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Maybe you can see one in one of the museums of natural history of science in Turkey.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
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