00:01
The first thing we should do for this question is draw a diagram.
00:03
And a diagram of mars with respect to our telescope and the light going in.
00:07
So we know that mars will send light through our telescope about, you know, horizontally like that.
00:16
And you would expect to also send light from the top through our first objective lens like that.
00:25
And we know the resulting image will be something of the source.
00:31
Of this red arrow or this red block there.
00:36
And we know that this occurs at the focal length of our first lens, or our eye piece actually, so i'm just gonna do fi.
00:47
And because of this, the image produced by the objective lens becomes parallel rays that we can then look through with our eyes.
00:59
But we know that this let's see if i can get it.
01:05
This angle here is our theta i, which we are given, and we know this angle here is the same as this angle, which makes it theta objective.
01:17
So if you can recall the equation, total magnification of a telescope is equal to theta i over theta objective, which is equal to negative f objective over fi, then we can express f objective while ignoring the negative signs...