"" <> writes:
>You have used a legitimate method to calculate the
>35 mm equivalent focal lengths by linear proportions.
>By using linear proportion, all the "form" factors
>are automatically included. This method is good enough
>for all practical purposes. However, strickly speaking
>this method is correct if the aspect ratio is the same
>and the normal focal length is equal to the diagonal.
No, it doesn't matter what the normal focal length is considered to be,
since that doesn't need to enter the calculations at all.
If the aspect ratios of the two formats are different, then you have to
make it clear whether you are calculating "equivalent" focal lengths by
making the horizontal FOV, the vertical FOV, or the diagonal FOV the
same. There are 3 different answers depending on which you choose to
make equal.
>Let us go through the "formal" exercise in calculating
>the 35 mm equivalent. The diogonal of the sensor of 7.2 mm
>width is 9 mm. The normal focal length of this sensor is
>9 mm (strickly by definition). 7/9 = .7778 and 21/9 = 2.3333.
>So the 35 mm equivalent is 39 - 117 mm based on 50 mm and 33
>- 100 based on 43 (which nobody uses now). You can see that
>what normal focal lengths to use does matter if you follow
>the "formal" procedure.
I've never seen that particular procedure used before. You're
converting every focal length into a ratio against the normal lens for
the one format, then multiplying that by the normal lens for the other
format. That does give you a sort of "comparative" focal length, but it
doesn't give you the same field of view unless the two normal FLs are
carefully matched!
Instead, here is the usual method of focal length conversion: scale
focal lengths proportional to sensor dimensions to preserve FOV.
For example, suppose we want to preserve horizontal FOV. The sensor
width is 7.2 mm, while full frame width is 36 mm. So focal lengths of 7
and 21 mm on the digital camera are equivalent to 7 * 36/7.2 = 35 and
21 * 36/7.2 = 105 mm. These are exactly equivalent, in terms of
matching horizontal FOV.
If you want to match diagonal FOV instead, the diagonal of a 7.2 mm wide
1.333 aspect sensor is 9 mm, the diagonal of a 36 mm wide 1.5 aspect
ratio 35 frame is 43.27 mm, and the multiplier to convert from true FL
to "35 equivalent" FL is 4.8 instead of 5.0.
But none of these calculations depend on what is considered "normal" for
either format.
>The best way to record the telescope image is to directly
>expose it on the sensor of a DSLR. Since we cannot remove
>the lense of a P&S digicam, one way is to "relay" the
>image to the sensor by using a "relay lense" formed by the
>eyspiece and the lens of the camera. This is normally done.
>In doing so there is a "final" magnification/demagnification
>depending on the focal ratio of the two. It is best to see this
>by the following experiment (theoretical or physical). Align
>two lenses of equal focal length on their optical axis. If you
>put an image at the first lens and an image of equal size
>(inverted) is formed at the focal plane of the second. If you
>double (or halve) the focal length of the second lens, the image
>is doubled (or halved). I did not discuss the many technical
>details which you discussed some. The operation the relay lens
>is just like this.
Ok. But, in general, it's not desirable to make the FL of the camera
lens equal to the FL of the telescope eyepiece. That *is* true if
you're trying to simulate the effect of removing the lens from the
camera, removing the eyepiece from the telescope, mounting the camera
directly on the telescope, and doing "prime focus" photography.
But if you leave the eyepiece and camera lens in place, you generally do
not want 1:1 relaying. You want to relay most of the image that the
eyepiece "sees", whose real size is set by the field stop inside the
eyepiece, onto the sensor in the camera. For a given eyepiece and field
diameter, this means that the camera lens FL should be proportional to
the size of the camera sensor. Put another way, you want the camera to
capture a particular field of view, no matter whether that's a 14 mm FL
on a small digicam or a 70 mm FL on a full-frame SLR.
So you're right: the magnification of the "relay optics" is determined
by the ratio of their focal lengths. Doing calculations with these, you
need to determine how the objective's FL converts an angle at infinity
into a distance in the primary focal plane, and then use the relay
optics magnification to convert that to a distance on the sensor, which
ultimately becomes a distance on the print given the printing
magnification.
In contrast, I was keeping things in the angular domain as long as
possible. The telescope objective and eyepiece together provide an
angular magnification, and this angle is a certain portion of the FOV of
the camera. The two methods are equivalent and should give the same
ultimate answer.
Dave
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