1 99:59:59,999 --> 99:59:59,999 So how do we know that there is a core 2 99:59:59,999 --> 99:59:59,999 that the core is made up of a liquid outer core and a solid inner core 3 99:59:59,999 --> 99:59:59,999 and the answer there coems from the same technique that we saw use. 4 99:59:59,999 --> 99:59:59,999 in 1909 to essentially see how the behaviour or when you measure the siesmis waves 5 99:59:59,999 --> 99:59:59,999 or whether you can even measure the siesmic waves the different distances 6 99:59:59,999 --> 99:59:59,999 from and earthquake. So if there is an earthquake right here and we are calling that 0 degrees 7 99:59:59,999 --> 99:59:59,999 let's remember a couple of things right here. Let's remember that p-waves can travel 8 99:59:59,999 --> 99:59:59,999 through anything. They can travel through solids or liquid or air for that matter. 9 99:59:59,999 --> 99:59:59,999 So they can travel through anything. 10 99:59:59,999 --> 99:59:59,999 But s-waves can only (s for secondary) s can only (these are the transverse waves) 11 99:59:59,999 --> 99:59:59,999 these can only travel through solids. So turns out that if an earthquake happens at 12 99:59:59,999 --> 99:59:59,999 0 degrees and you have seismograph stations all over the world 13 99:59:59,999 --> 99:59:59,999 and these are extrememly sensitive in order to measure earthquakes that are happening 14 99:59:59,999 --> 99:59:59,999 thousands of kilometres away. It turns out that there is something called an s shadow 15 99:59:59,999 --> 99:59:59,999 and s waves shadow. You can measure them here, you can measure them here 16 99:59:59,999 --> 99:59:59,999 They can go over there, they can go over here you can measure them over here. 17 99:59:59,999 --> 99:59:59,999 You see measurement in all of these points but then suddenly 18 99:59:59,999 --> 99:59:59,999 at 105 degrees. We are measuring 0 degrees here and we are going outwards like that. 19 99:59:59,999 --> 99:59:59,999 Suddenly at 105 degrees you stop measuring s-waves 20 99:59:59,999 --> 99:59:59,999 For soem reason you think that the s-waves would get over here. 21 99:59:59,999 --> 99:59:59,999 That they would get over here, maybe a little bit weaker 22 99:59:59,999 --> 99:59:59,999 but they would be able to get all the way over here. 23 99:59:59,999 --> 99:59:59,999 But they just abruptly stop. No more s-waves 24 99:59:59,999 --> 99:59:59,999 So in this whole area right over here you get no more s-waves 25 99:59:59,999 --> 99:59:59,999 And obviously I could flip this picture over 26 99:59:59,999 --> 99:59:59,999 and you would get see a symetric thing on the other side of the globe 27 99:59:59,999 --> 99:59:59,999 All over here you would not see s-waves 28 99:59:59,999 --> 99:59:59,999 You would only see them from 105 degrees in this direction and 105 degrees in that direction 29 99:59:59,999 --> 99:59:59,999 and the only reasonable explanation that we could give 30 99:59:59,999 --> 99:59:59,999 is that there must be some material that an s-wave cannot travel thorugh 31 99:59:59,999 --> 99:59:59,999 that is would have to travel through to get to these points beyond 105 degrees 32 99:59:59,999 --> 99:59:59,999 and we know that s-waves only travel in solids. 33 99:59:59,999 --> 99:59:59,999 So the assumption there is that at some point beyond 105 degrees 34 99:59:59,999 --> 99:59:59,999 it's hitting liquid. 35 99:59:59,999 --> 99:59:59,999 So that's what tells us that this right here is probably a liquid 36 99:59:59,999 --> 99:59:59,999 So that tells us that there is a core and that at least the outer part of that core is 37 99:59:59,999 --> 99:59:59,999 liquid enough to stop s-waves. 38 99:59:59,999 --> 99:59:59,999 So the s-waves because they only travel in solids it leads to this s-wave 39 99:59:59,999 --> 99:59:59,999 shadow and this tells us that we have a core and that core at least the outer part 40 99:59:59,999 --> 99:59:59,999 is liquid 41 99:59:59,999 --> 99:59:59,999 we don't know yet whether the inner part is liquid or solid. 42 99:59:59,999 --> 99:59:59,999 Not the next point of emphasis is how do we know 43 99:59:59,999 --> 99:59:59,999 that there is an inner core? 44 99:59:59,999 --> 99:59:59,999 We could use p-waves for that 45 99:59:59,999 --> 99:59:59,999 The p-wave, a p-wave can travel through anything. 46 99:59:59,999 --> 99:59:59,999 But remember as you get denser material 47 99:59:59,999 --> 99:59:59,999 In general for the same type of material 48 99:59:59,999 --> 99:59:59,999 if you get denser material its going to move faster 49 99:59:59,999 --> 99:59:59,999 so its going to refract outwards like we see here 50 99:59:59,999 --> 99:59:59,999 but if it goes into a iquid in general sound waves or as I should say p-waves 51 99:59:59,999 --> 99:59:59,999 or seismic waves will move slower in liquids 52 99:59:59,999 --> 99:59:59,999 and so the refraction patterns that we get 53 99:59:59,999 --> 99:59:59,999 when we do measure from seismograph stations around the world