00:01
We're told that a column of air, and we're given the temperature.
00:06
So that tells me that the speed of sound is going to be 340 meters per second.
00:18
And it's got frequencies with no frequencies between them.
00:22
So if i just subtract any two of the frequencies, let's say, 520 minus 390, that'll give me the fundamental frequency of 130 hertz.
00:55
So we're asked whether this is open, open, or open, closed.
01:10
So i think i may have jumped a little bit to finding the frequencies.
01:20
I was assuming that it was close, closed.
01:32
All right.
01:32
So i did jump to conclusions there.
01:36
However, i noticed the following, and perhaps this is why i jumped to that conclusion.
01:49
650 minus 520 hertz is 130 hertz.
02:16
Minus 390 hertz is also 130 hertz.
02:23
I'm gonna keep subtracting off 130 hertz.
02:27
I'm gonna keep subtracting off 130 hertz.
02:28
So 390 minus 130 gives me 260 hertz.
02:39
So the next, the previous frequency would be 260 hertz.
02:49
And if i subtract off 130 again, i get 130.
02:58
Since these are consistent the whole way, then it is indeed open open.
03:08
And the fundamental frequency is 130 hertz.
03:21
B, how long is the tube? so to figure out the length of the tube, we just have to set the fundamental frequency equal to v over to l.
03:37
So l is going to be v over 2f1.
03:44
Let me put that in a calculator.
03:49
340 meters per second over 2 times f1, which is 130.
03:55
The tube, looking for significant digits here, looks like two to me.
04:04
I think the numbers are given to us in two significant digits.
04:07
And so 1 .3 meters.
04:19
Moving on to see.
04:24
Displacement graph of the 520 hertz standing wave.
04:34
Okay, well, this is the fundamental frequency here.
04:39
It should be second, third, fourth.
04:43
So i need to draw four nodes because this is over.
04:52
This is going to be the number of nodes.
04:56
And so, anti -node at the beginning, one, two, three, four nodes.
05:11
Okay...