Next message: Mike Hannibal: "Re: Sextants with Polarizing filters"
> From: George Huxtable
> Some things I don't understand about Peter Fogg's recent message are
>
> 1. How can you reduce the brightness of light by more than 100%? If you
> have reduced it by 100%,
> then you have already achieved complete darkness.
An f/stop more is a doubling of light brightness, thus 100%, while an f/stop
less is a halving, thus indeed 50%. A somewhat pedantic point hardly worth
making, I would have thought.
>
> 2. Yes, if you introduce one polarising filter, you will approximately
> halve the light intensity,
> for initially unpolarised light, because you are excluding the 50% of the
> light that is polarised at
> right angles to the direction of the filter that lets light through. Plus
> a slight further
> reduction, to allow for losses in the plastic material and in surface
> reflections.
>
, that
> won't halve the light intensity again, because now all the light entering
> it is polarised in the
> preferred direction. This second filter will therefore cause a slight
> reduction in intensity, as
> before, because of further losses in that extra layer of plastic and
> further reflections, but
> nothing like the reduction that the first filter caused. That's a
> deduction based on theoretical
> reasoning, not on any practical tests by me, so it may possibly be
> contradicted by experiment. I
> would be interested to learn if it is.
Take two polarising filters and try it out, George, as suggested by me
earlier (I do hope it was included in the part you did understand). Once you
see it working, more convoluted reasoning may be introduced to explain how
it does, perhaps..
> ... if you add a second filter, that's polarised in the same
> direction as the first ...
By turning the second filter the remaining light polarised in the other
direction is gradually choked off until no light passes.
Getting back to sextant filters, the advantage is that the intensity of
light passed by the two filters is infinitely adjustable, with, again; the
proviso that the initial minimal light diminution is not.
