Back to Alaska Airlines Plebs Status


I missed reaching Alaska Airlines MVP this year by 652 miles — not to be confused with the time I missed MVP Gold by 2000 miles. I thought about making a year-end milage-run, a process where you “[buy] a low-price airline ticket … and fly not because you want to go anywhere, but to earn redeemable miles and progress toward elite status on your preferred airline.”

Alaska_Airlines_Boeing_737-800_CThe benefit of MVP is free checked bags for myself and Rachel (when she flies with me), which can easily save us $50-$100 per a trip. I also would get first crack at awesome seats such as 6A/F and 17A/F.

If I had been on top of my game, I probably could have accrued the required miles for about $200, which is equivalent to 2-4 trips worth of baggage fees. Realistically, I think there will only be a couple of flights we take this year (Colorado in August, and maybe someplace warm in the spring). This kind of makes it a push in terms of value. Unfortunately, I left it to the last few weeks of the year and it was going to cost upwards of $400 to get a flight that worked with my schedule. C’est la vie.

I suppose the good news is that I’m not traveling as often…though I sometimes miss it.


What’s your Critical Level to Get Things Done

For me, it’s two.

I’ll often make decisions when some level reaches two.

If I need to email someone about something, I won’t email them if it’s just one thing. But I have to ask them about two or point things, I’ll do it.

If a request is made to add a feature, I may not add it if only one person requests it, but if I get two requests, then I usually do.


Stupid People, Stupid Questions, and the Lazyweb

  • Rants

Scott Adams has a great quote:

If there are no stupid questions, then what kind of questions do stupid people ask? Do they get smart just in time to ask questions?

This quote came to mind as I was reading a post by Jeff Atwood on the word Lazyweb:

It’s hard to pin down the exact etymology of the word Lazyweb, but it seems to have one primary meaning:

1. Asking a question of an internet audience in the hopes that they will be able to find a solution that you were too lazy or inexperienced to find yourself.

I don’t mind Lazyweb requests, within reason. Contrary to popular belief, there is such a thing as a stupid question. It’s asked by people who failed to do even the most basic kind of research on their question before they asked. I’m not expecting everyone to read a 32 page document before asking a question, but at least cover the basics before casually deciding to make your problem everyone’s problem.

My wife can attest to my love of answering questions, especially engineering/technology questions. At the same time, one of my biggest pet peeves are questions which are asked simply because the asker has not done any level of work to answer the questions himself1.

For a while, I used to respond to such questions with my Larry and Sergey story. Ask me a lazyweb question sometime and I’ll tell you my story.

When I needed help from a professor in college, I learned to preface the question with a synopsis of what I had done thus far in my attempt to answer it. This seemed to help direct their answers more specifically to my particular failure of knowledge, as well as assure them that I wasn’t being lazy.

  1. please do not ask me what time it is, I’m pretty sure you have a cell phone with a clock on it 

In Greek legend, Icarus flew too close to the Sun,…

In Greek legend, Icarus flew too close to the Sun, and the heat melted his wings and he fell to his death. But “melting” is a phase change which is a function of temperature, a measure of internal energy, which is the integral of incident power flux over time. His wings didn’t melt because he flew too close to the Sun, they melted because he spent too much time there.

Visit briefly, in little hops, and you can go anywhere.


Somebody once told me, “Manage the top line, and t…

Somebody once told me, “Manage the top line, and the bottom line will follow.” What’s the top line? It’s things like, why are we doing this in the first place? What’s our strategy? What are customers saying? How responsive are we? Do we have the best products and the best people? Those are the kind of questions you have to focus on.


Space Moon

Space Moon
800.0 mm || 1/13 || f/5.6 || ISO3200 || NIKON D7000
Seattle, Washington, United States

If you just want to look at a pretty picture, you can stop now. If you’re curious about how this picture came about and are not afraid of some math, keep reading.

The Idea

Cool picture, right? Here’s what went into making it:

It all started with an email to my friend Jacob, who moved back to Alabama1 last year:

Remember when I rented that 600mm lens for Seafair a couple years ago?
I’m renting the 800mm this year…wish you were here.

On my DX body, it’s effectively a 1200mm and it also comes with a 1.25 teleconverter for 1500mm of awesomeness.

While the primary intent was to take pictures at Seafair, Jake and I went back and forth for a bit on other cool photo ideas, originally talking about astrophotography but then moving to something a bit more Earth-bound. The idea was to do an ET-esque moonshoot similar to what Switzerland-based photographer Philipp Schmidli did:

The Silhouette of a Bike Rider on Thursday, April 25, 2013 before the rising full moon. Photo by  Philipp Schmidli.

The Silhouette of a Bike Rider on Thursday, April 25, 2013 before the rising full moon. Photo by Philipp Schmidli.

Another friend, Nate, was having a bachelor party that would involve lots of biking on Friday night. I was hoping to get everyone biking on top of the hill at Gas Works park, but the technical logistics don’t really work. Let’s go through the data.

The Data

Here’s the US Naval Observatory (USNO) Calculated Altitude/Azimuth Data for the Moonset times (when the Moon is at an altitude2 of 0°):

Date Time Azimuth3 Fraction Illuminated
8/1 23:00 258.1° 0.32
8/2 23:29 252.6° 0.42
8/4 00:02 247.7° 0.53

For Friday (8/1), the reverse bearing is 258.1^{\circ} - 180^{\circ} = 78.1^{\circ}. Moving out 1000 meters4 from the Gas Works Park hill (“S”) on a bearing of 78.1° puts us right over by I-5 (“D”) — so at least we’re on land.


Gas Works Park hill (“S”) on a bearing of 78.1° puts us right over by I-5 (“D”)

Unfortunately, it also puts us at an elevation that’s ~30 meters above the top of the Gas Works Park hill — we’d be looking down at them by \textup{tan}^{-1}\left ( \frac{-30\textup{m}}{1000\textup{m}} \right ) = -1.718^{\circ}:

Note: the elevation profile (top) is the opposite direction as the map (bottom).

Moving down to the water would reduce our elevation, but now we have another problem: Queen Anne Hill is blocking the moon. We’d have to shoot looking up 2.5°: \textup{tan}^{-1}\left ( \frac{65\textup{m}}{1500\textup{m}} \right ) = 2.481^{\circ}

Note: the elevation profile (top) is the opposite direction as the map (bottom).


Going back to the USNO, we could look up and find that at 22:43 the Moon will be at an elevation of 2.5° and an azimuth of 255.0°, or about 3.1° to left of where it would be at 23:00. We could keep playing this game until we found the perfect spot, but that still doesn’t solve our issue of being too close to the subject (i.e. the bikers at Gas Works Park).


The Gas Works Park location does not work because we must be far enough away from our primary subjects (the bikers in this instance) for them to appear small enough in comparison to our secondary subject (the Moon). Just how far is a function of \textup{tan}\ \theta = \frac{opposite}{adjacent} (Or solving for theta: \textup{tan}^{-1}\left (\frac{opposite}{adjacent} \right ) = \theta, which is the equation used several times above)


The tangent of an angle is the ratio of the length of the opposite side to the length of the adjacent side.

In order to make the primary subject look smaller in comparison to the Moon, we are taking advantage of the fact the arc length (θ) of an object does not change significantly when your distance from the object is very large in comparison.

Arc diameter (Y-axis) vs ratio of distance/diameter (X-axis, log plot)

For example, the diameter of the Moon is about 3,475 km and the distance from the Earth to the Moon is about 385,000 km. This means the Moon has an arc diameter of:  \textup{tan}^{-1}\left ( \frac{3475 \textup{km}}{385000 \textup{km}} \right ) = 0.5171^{\circ}

Even if we move 100 km toward the Moon the arc diameter would still only be:  \textup{tan}^{-1}\left ( \frac{3475 \textup{km}}{385000 \textup{km} - 100 \textup{km}} \right )= \textup{tan}^{-1}\left ( \frac{3475 \textup{km}}{384900 \textup{km}} \right ) = 0.5173^{\circ}

…a difference of 0.0002°

Meanwhile, a person 1.8 m tall at a distance of 1 km would have an arc height of: \textup{tan}^{-1}\left ( \frac{1.8 \textup{m}}{1000 \textup{m}} \right ) = 0.1031^{\circ}

However, if we move closer just 0.5 km the person now has an arc height of: \textup{tan}^{-1}\left ( \frac{1.8 \textup{m}}{1000 \textup{m} - 500 \textup{m}} \right ) = \textup{tan}^{-1}\left ( \frac{1.8 \textup{m}}{500 \textup{m}} \right ) = 0.2063^{\circ}

…a difference of 0.1°!

Math with Bicycles

In Schmidli’s Moon photo, the Moon is about 7 bicycles in diameter:

If the bicycle is 1.8 m long, the camera must be at a distance of: \textup{tan}^{-1}\left ( \frac{3475 \textup{km}}{385000\textup{km}} \right ) = 7*\textup{tan}^{-1}\left ( \frac{1.8\textup{m}}{x}\right ), where x is the distance between the primary subject (the bicyclist) and the camera. Solving for x\Rightarrow x = \frac{9}{5} \textup{cot}\left (\frac{1}{7} \textup{tan}^{-1} \left ( \frac{139}{15400} \right) \right) \approx 1396.0

…1.396 kilometers.

If Schmidli had only been 500 meters away, the photo would have probably looked something like this:

It still looks cool, but not as cool. So, what else could I take a picture of?

Another Idea

How about the Space Needle? Plotting the azimuth of the Moon set for all three nights to see if a good location is feasible:


Bearing of the Moon set on 8/1, 8/2, and 8/4

The southwest corner of Volunteer Park on Sunday, August 4th looks like it could work and the elevation profile looks good too:

Note: the elevation profile (top) is the opposite direction as the map (bottom).

The “Black Sun” sculpture at Volunteer park is at ~137 m above sea level and the base of the Space Needle is ~2.77 km away at ~40 m above sea level. The top floor of the Space Needle is ~158 m above ground level which makes the top floor 198 m above sea level. Google Street View confirms that we have good view. I stopped by during the day to confirm the view and find a good spot to setup.


Framing the Picture

The Space Needle “Halo” has a diameter of ~42 m which at a distance of 2.77 km gives it an arc diameter of \textup{tan}^{-1}\left ( \frac{42 \textup{m}}{2770 \textup{m}} \right ) = 0.8687^{\circ} — or about 1.7x larger than the Moon. The maximum angle of view of the Nikkor 800mm (on a DX body) is just 2° — thus the Space Needle should take up about 43% of the frame width.

I relayed my findings back to Jake:

I’ve been doing some math, and on Sunday night I’ll head to up to the SW corner of Volunteer Park. That puts me on a 248 deg bearing with the space needle and the moon will be right behind it. At 2500m away, the halo of the space needle will still appear to be about twice the diameter of the moon and if I put the teleconverter on I think the moon + spaceneedle will fill the frame just about perfectly.

So something like this…but in high def:

So that was that. I showed up a bit past 11pm on the night of August 3rd, set up my equipment, and sat around listening to passersby play the piano as they filtered out of the park. I took test photos as the Moon grew closer and closer, and then just like clockwork…almost.

Lessons Learned

I forgot to take into account the height of Space Needle relative to the elevation of the Moon, so the Moon was too far to the left for the picture I was hoping for — but pretty much dead on the calculations I made, even if I calculated the wrong thing.

The halo of the Space Needle was at an elevation of \textup{tan}^{-1}\left ( \frac{198 \textup{m} -137 \textup{m}}{2770 \textup{m}} \right ) = 1.262^{\circ}. Add 0.3° for the arc radius of the Moon to get ~1.6° of elevation. Using the USNO table, we find the Moon at an azimuth of 245.6° at 23:50. The reverse bearing is 65.6° which puts me about 100m too far south-ish for the picture I wanted. Unfortunately, the right spot was blocked by trees…so it’s kind of a moot.

Making Lemoonade

Put I still have a bunch of really cool photos and after looking at them all of a bit I think to myself, “Hmmm…this could be really cool as a multiple exposure / panorama shot.”

I went through all the photos to find the ones that had both a complete view of the Moon and at least part of the Space Needle. Three interesting things occurred as the Moon started to set:

  1. The Moon became more red as it set. This is due in part to particulates in the air (e.g. pollution) as well as atmospheric scattering (i.e. Rayleigh scattering).
  2. The luminance of the Moon decreased significantly during its setting, such that its exposure was almost the same as the Space Needle. The Moon is typically several stops above the ambient landscape, even when the landscape is lit up. If you’ve ever tried to take a photo at night, you’ll probably notice that the Moon looks blown out — this is why.
  3. The shape of the Moon gets a bit wonky as comes in line with the ground and picks up some heat shimmer.

I played around with different sets of pictures and finally settled on a set that I think flows well. I did some basic exposure and color correction so that the photos were more-or-less “correct” and then imported them into Photoshop. Once in Photoshop, it was just a matter of aligning the images to build the panorama and then masking out sections to get the multiexposure.  The Space Needle itself is a composite of several different shots because I couldn’t fit the entire Space Needle into a single shot (yea, it’s a BIG zoom lens). I also needed a properly exposed shot of the interior of the top floor and a shot of the elevator in motion. Here’s what it looks like decomposed:


  1. Roll Tide 

  2. For the record: I prefer “elevation”, but I’ll try to remain consistent with the USNO wording 

  3. E of N 

  4. at this point, 1000 m is just an arbitrary “best guess” for how far away I’d have to be