00:01
So we have a mercury bulb, let's say the volume of the mercury bulb was v, which we know is 0 .275 centimeter cubed.
00:12
And let's say the mercury was until a length l0 and it goes to delta l after the expansion.
00:22
The temperature went from 10 .5 degrees to 33 degrees, which means a delta t of 22 .5 degrees degrees.
00:38
Now, so when the temperature changes, the glass bulb expands and the hg, the mercury inside also expands.
00:53
So the total extra liquid that will flow into the cube would be the change in the volume of mercury minus the change in the volume of glass bulb because the extra volume of glass bulb would accommodate a little of the extra mercury volume.
01:13
So the net increase in the volume in the tube would be, let's say, delta v.
01:26
That would be delta v hg minus delta v glass, which would correspond to the volume of the bulb, beta of mercury, delta t minus volume of the bulb, beta of glass, beta of delta t, minus volume of the bulb, beta of glass times delta t.
01:43
Now, to find this length delta -l, we know that surface area of the tube, let's say it is a, the length, the changing length times the surface area must be equal to delta v, which gives us the change in length is equal to delta v by the area.
02:04
We know that the diameter is 0 .140 millimeters, which means area must be 5d square by 4.
02:15
Now, you know that delta v is this.
02:18
So let's use that...