Transcript

TOM:

Welcome to next practical we're going to do, which is based on the laser pen of different wavelengths and also some diffraction gratings as well. The first diffraction grating we're going to look at is of order 600 lines per millimetre. Then we're going to look at one which has 300 lines per millimetre.

What we're going to do is show that light can behave like a wave as well as a particle. And for that we need, this important equation up on the board here, n lambda equals d sin theta. We'll be looking at what we changed is how it's going to affect the outcome. So we'll have a wave length and an angle here as well.

For the first part of the practical, we've got a blue laser, and we're going to put it through a diffraction grating here of 600 lines per millimetre. And the blue laser, as it goes through, has spots that come up to the centre, to the left, and to the right. Helen will mark these spots as we go through and see the one in the centre and three to the left.

Now number them 1, 2, and 3. That's the order from the centre is naught, 1, 2, and 3 to the left. That's from the blue laser.

Now what would happen if we changed the colour of the laser? We're now going to go for different colour laser. And again, we're going to use the same diffraction grating, and we're putting a green light through the same diffraction grating.

Now you'll see with a different colour, the spots are in different locations. The one at number 1, number 2 have moved slightly more.

Now we'll change the colour of the laser. Now let's try red coloured laser going through the centre of the 300 lines per millimetre diffraction grating. You see it's quite hard to see the next spot with the red laser.

Now we've used different laser pens with the same diffraction grating. We're now going to change the diffraction grating from 600 lines per millimetre to 300 lines millimetre.

I will start back with the blue coloured laser, I'm going to move that one out of the way. And we'll move. We're now with the blue laser going into diffraction grating of 300 lines per millimetre.

Now you see with the locations of the blue spots in the middle, and the blue spot compared before has now moved considerably to the right, the closer to the centre. So now the numbers being marked up are number 1, number 2 are closer to a centre. Do we expect that to happen for the other coloured lasers? Let's have a look.

You remember last time on the 600 line millimetre, we had number 1 to the left, and again, we've got number 1 to the left, which is much closer to the centre than before. Now we have number 1, number 2, number 3, number 4, and even number 5.

And finally, for the last laser, again, we can make our expectations of what's going to happen. And we'll try that with the same, with a red laser, and we'll see again the spots have moved to the left in comparison with number 1 before.

The conclusion of what we've done here is we look through the material in the course as we're working through. And the conclusion is the laser going through diffraction gratings of different number of lines per millimetre is affected by the equation n lambda equals d sin theta. If you change one thing, you will change the outcome of your experiment.