00:01
In this problem we have two questions which are all related to some uncertainties.
00:09
And let's get started with the first one.
00:14
Here we are asked to give two at least two reasons for the sources or the reasons of uncertainties in measurements.
00:27
So actually there are two sources of uncertainty.
00:30
So let me just write them down.
00:35
Sources of uncertainties in measurements.
00:43
The first one is the limitation of the measuring instrument.
00:51
Limitation of the measuring instrument.
01:04
And the second one is the skill of the experimenter who performs this measurement.
01:17
So it's a human issue, basically.
01:21
So skill of the experimenter performing the measurement.
01:39
So these are our two sources of uncertainties in measurements.
01:47
Now, let us do the second one.
01:50
Second question.
01:52
We have two numbers that contains some errors.
01:55
So x equal to some x bar plus minus delta x.
02:01
So i am writing it in this form so that you know my notation.
02:06
So we have y equal to y bar indicating that it is a central value plus minus delta y.
02:14
Then we define this quantity z to be x plus y.
02:20
And we are going to compute the central value of this z number and the upper bound of the delta z, namely the error of this number.
02:34
So it's express this x bar plus minus delta z.
02:41
So z bar is simply given by x bar plus y bar.
02:48
So we have 2 .5 plus 3 .1 centimeters.
02:57
So this is just 5 .6 centimeters.
03:07
And we have this delta z given by delta x squared plus delta y squared.
03:21
Okay, maybe i should put some parentheses here so that these are the squares of errors, not the errors of the squares.
03:30
So this is 0 .1 squared plus 0 .1 squared and we have this huge number 0 .1 .1421 centimeters.
03:50
I am writing this in this form to point out to point out to something.
04:00
We have z equal to 5.
04:04
6 plus minus some error...