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March 9

Feynman Lectures. Lecture 15 (34). Special relativity [1][2]

We have the Lorentz transformation:
x=xut1u2/c2,y=y,z=z,t=tux/c21u2/c2,
Suppose a man Joe in S reference frame measures coordinates of some point A at t=0. In S the point A has coordinates:
A(x,y,z).

From Joe's point of view a moving (in positive x direction) man Moe in his reference frame S at t=0 has coordinates:
A(x,y,z)=A(x1u2/c2,y,z).

But from Moe's point of view A is moving with speed u. So his coordinate x contracts to x1u2/c2.

Moe can highlight a position of A on his x-axis. What will see Joe ? Will he see 2 highlighted marks x1u2/c2 and x1u2/c2 ?


Username160611000000 (talk) 14:04, 3 March 2019 (UTC)

I'm having a hella time following that, but I think what you're saying is that if you look at a Lorentz-contracted object and imagine how far that object thinks it has gone past you, you suppose that because it is contracted it thinks you are expanded. But in truth the object sees you as contracted as much as it is, so the distance is contracted in both frames! The reason is that you and it don't see the same times as simultaneous. You could highlight the same point at different times, but that shouldn't be sufficient to actually expand the distance to x*gamma factor; when two points are at relative rest, and the distance between them is x in that frame, it won't be longer than that in any frame, I don't think.  ??? Wnt (talk) 17:12, 3 March 2019 (UTC)
Template:ReTemplate:Tq Both men stay at coordinates x=x=0;t=t=0. The only difference is that they move relative to each other, and point A is at rest in system S. Username160611000000 (talk) 18:24, 3 March 2019 (UTC)
The time coordinates are:
in S: A(x,0);
S as seen from S: A(x,t)=A(x1u2/c2,ux/c21u2/c2);
in S (as seen from S): A(x,0)=A(x1u2/c2,0);
S as seen from S: A(x,t)=A(x,+ux/c21u2/c2).
t=t' *only* where x=x'=0. Wherever x != x', now one of the times is nonzero relative to the other. Wnt (talk) 12:34, 4 March 2019 (UTC)


In the Lecture 34 Feynman says Template:Quote frame Why have we to divide by 1v2/c2 ? Is it because a moving person thinks that time t (or better Δt ) has passed at a slow clock rate? The moving man takes Δt from S , converts it to his time Δt=Δt/1v2/c2 and then does he take the same radians and divide? Username160611000000 (talk) 09:52, 8 March 2019 (UTC)

Mute swan wings

I've noticed there's a particular way mute swans and some black swans swim, with their wings partially raised off of their backs. This is in contrast to the trumpeter swan, which holds its wings completely folded while swimming. Is there a specific name for what these birds are doing? Template:Gallery BlueSkinnyJeans (talk) 02:45, 9 March 2019 (UTC)

(Reformatted your image list.) --76.69.46.228 (talk) 05:46, 9 March 2019 (UTC)
By raising the profile of theirs wings the Mute swan and the Black swan are exhibiting threatening or assertive behaviour. Swans under non-threatening circumstances will swim with the wings flat against the body but in response to a perceived threat, particularly when protecting young or a nest, will raise their wings which increases the apparent size of the bird. Wing raising as a threat in Trumpeter swans seems much rarer or possibly non existent. I was unable to find any image to demonstrate it. Richard Avery (talk) 09:21, 9 March 2019 (UTC)
It's called "busking". [3] Alansplodge (talk) 14:50, 9 March 2019 (UTC)
Then I suggest a short article busk (birds) or busking (birds). --76.69.46.228 (talk) 06:40, 10 March 2019 (UTC)
Or, since it only seems to be associated with swans, maybe just a section in the swan article? Or in Display (zoology)? —107.15.157.44 (talk) 07:43, 10 March 2019 (UTC)
National Geographic suggests they may also use this posture to "windsurf" across water: [4]107.15.157.44 (talk) 08:07, 10 March 2019 (UTC)