http://www.skyandtelescope.com/observing/home/232699581.html
We haven't chatted about it in class - it's an early morning object, and not terribly bright yet. Still, it *may* end up great. Nobody seems to be sure.
Wednesday, November 20, 2013
FYI - observation night and optics
Observation night is: December 5, 7 PM. Backup night: December 10, 7 PM
Here's the lens applet I was playing with today in class:
http://www.physics.metu.edu.tr/~bucurgat/ntnujava/Lens/lens_e.html
Here's the lens applet I was playing with today in class:
http://www.physics.metu.edu.tr/~bucurgat/ntnujava/Lens/lens_e.html
Hella-cool!
Interactive supernova
http://54.225.120.196/tour/seeing-around-remnant-supernova
A bit of background:
http://www.skyandtelescope.com/news/Cassiopeia-A-in-3D-232367901.html
http://54.225.120.196/tour/seeing-around-remnant-supernova
A bit of background:
http://www.skyandtelescope.com/news/Cassiopeia-A-in-3D-232367901.html
Monday, November 18, 2013
Today
Folks,
I can't come in until around 11:30 today, so I have to miss our class. Please work on the following stuff:
If you have not done the blog homework from the weekend, do so. Also, check out some recent blog posts, most of which were there for your information (such as the full Moon names). If you want to look ahead, read my notes on stellar classification and the H-R diagram (though we'll cover this in our next class).
Find out how realistic it will be for us to see Comet Ison this fall - when will it be visible.
Then, work through this simulation online. Use the computer lab next door, computers upstairs or in the library, and/or any personal computers.
http://wechoosethemoon.org/
See you Wednesday.
I can't come in until around 11:30 today, so I have to miss our class. Please work on the following stuff:
If you have not done the blog homework from the weekend, do so. Also, check out some recent blog posts, most of which were there for your information (such as the full Moon names). If you want to look ahead, read my notes on stellar classification and the H-R diagram (though we'll cover this in our next class).
Find out how realistic it will be for us to see Comet Ison this fall - when will it be visible.
Then, work through this simulation online. Use the computer lab next door, computers upstairs or in the library, and/or any personal computers.
http://wechoosethemoon.org/
See you Wednesday.
Thursday, November 14, 2013
Watch this / HW
http://www.upworthy.com/the-single-most-mind-altering-photograph-humanity-has-ever-taken
You may disagree with some of what Carl Sagan says, but you will probably at least find it poetic on some level.
And see this, mentioned in class today:
http://imgur.com/gallery/ylbWx7I
Cool:
http://www.iflscience.com/space/what-does-space-sound
Re: Comet Ison
http://earthsky.org/space/comet-ison-has-an-outburst
And other photos worth a look:
http://nssdc.gsfc.nasa.gov/planetary/lunar/apollo_11_30th.html
You may disagree with some of what Carl Sagan says, but you will probably at least find it poetic on some level.
And see this, mentioned in class today:
http://imgur.com/gallery/ylbWx7I
Cool:
http://www.iflscience.com/space/what-does-space-sound
Re: Comet Ison
http://earthsky.org/space/comet-ison-has-an-outburst
And other photos worth a look:
http://nssdc.gsfc.nasa.gov/planetary/lunar/apollo_11_30th.html
Reflection and Refraction
Reflection - light "bouncing" off a reflective surface. This obeys a simple law, the law of reflection!
The incident (incoming) angle equals the reflected angle. Angles are generally measured with respect to a "normal" line (line perpendicular to the surface).
Note that this works for curved mirrors as well, though we must think of a the surface as a series of flat surfaces - in this way, we can see that the light can reflect in a different direction, depending on where it hits the surface of the curved mirror. More to come here.
Refraction:
Refraction is much different. In refraction, light enters a NEW medium. In the new medium, the speed changes. We define the extent to which this new medium changes the speed by a simple ratio, the index of refraction:
n = c/v
In this equation, n is the index of refraction (a number always 1 or greater), c is the speed of light (in a vacuum) and v is the speed of light in the new medium.
The index of refraction for some familiar substances:
vacuum, defined as 1
air, approximately 1
water, 1.33
glass, 1.5
polycarbonate ("high index" lenses), 1.67
diamond, 2.2
The index of refraction is a way of expressing how optically dense a medium is. The actual index of refraction (other than in a vacuum) depends on the incoming wavelength. Different wavelengths have slightly different speeds in (non-vacuum) mediums. For example, red slows down by a certain amount, but violet slows down by a slightly lower amount - meaning that red light goes through a material (glass, for example) a bit faster than violet light. Red light exits first.
In addition, different wavelengths of light are "bent" by slightly different amounts. This is trickier to see. We will explore it soon.
The index of refraction is a way of expressing how optically dense a medium is. The actual index of refraction (other than in a vacuum) depends on the incoming wavelength. Different wavelengths have slightly different speeds in (non-vacuum) mediums. For example, red slows down by a certain amount, but violet slows down by a slightly lower amount - meaning that red light goes through a material (glass, for example) a bit faster than violet light. Red light exits first.
In addition, different wavelengths of light are "bent" by slightly different amounts. This is trickier to see. We will explore it soon.
Refraction, in gross gory detail
Consider a wave hitting a new medium - one in which is travels more slowly. This would be like light going from air into water. The light has a certain frequency (which is unchangeable, since its set by whatever atomic process causes it to be emitted). The wavelength has a certain amount set by the equation, c = f l, where l is the wavelength (Greek symbol, lambda).
When the wave enters the new medium it is slowed - the speed becomes lower, but the frequency is fixed. Therefore, the wavelength becomes smaller (in a more dense medium).
Note also that the wave becomes "bent." Look at the image above: in order for the wave front to stay together, part of the wave front is slowed before the remaining part of it hits the surface. This necessarily results in a bend.
The general rule - if a wave is going from a lower density medium to one of higher density, the wave is refracted TOWARD the normal (perpendicular to surface) line. See picture above.
http://lectureonline.cl.msu.edu/~mmp/kap25/Snell/app.htm
http://www.physics.uoguelph.ca/applets/Intro_physics/refraction/LightRefract.html
http://lectureonline.cl.msu.edu/~mmp/kap25/Snell/app.htm
http://www.physics.uoguelph.ca/applets/Intro_physics/refraction/LightRefract.html
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