Take the middle of each range:
| Source | σ (m) | σ² |
|---|---|---|
| Satellite clocks | 2.5 | 6.25 |
| Orbital | 0.8 | 0.64 |
| Ionosphere | 6.0 | 36.00 |
| Troposphere | 0.6 | 0.36 |
| Receiver noise | 0.9 | 0.81 |
| Multipath | 0.9 | 0.81 |
| Sum | 44.87 |
Same receiver, same sky, same instant — the geometry alone nearly triples the error.
Now redo it on your own paper with the low end of every range, and with PDOP = 1.5.



Each range is a band, not a line. Where the bands cross is your area of uncertainty.

High PDOP: satellites bunched together, large area of uncertainty. Low PDOP: satellites widely spaced, small area.
Two readings of the same point, one minute apart:





Reference deck. The Tuesday lecture uses the simplified "The Global Positioning System" deck, which already contains the Air Force One warm-up and the Prague activity. This deck keeps the longer material: the four-step position-fixing build, the error budget and PDOP arithmetic, and the latitude/longitude-to-meters demo, for anyone who wants the full story or for a semester with more time.
Say up front that they will be doing arithmetic today, not watching it. Have paper, calculators, rulers and a compass or a piece of string ready.
Two-minute recap. The one thing they need in hand for the next twenty minutes is D = R x T.
Worth thirty seconds because the vocabulary shows up on the quiz and in the reading. GPS never measures an angle to anything.
Four unknowns: latitude, longitude, height, and time. Four unknowns need four equations, which is why four satellites are the practical minimum. Start the build here and let it run through the next three slides.
The intersection of two spheres is a circle. Still an infinite number of candidate positions, but a much smaller infinity.
Three spheres intersect in exactly two points, and one of them is almost always absurd: out in space, or moving at an impossible speed. In practice three ranges are enough to fix a position.
The fourth range is not really about geometry, it is about the clock. Your receiver has a cheap quartz clock, not an atomic one, so its clock bias is a fourth unknown. The fourth satellite is what lets the receiver solve for it.
Leave this up while students work. A single measurement places the observer somewhere on the sphere; two place them on a circle; three place them at one of two points; knowing you are also on the surface of the Earth, a fourth sphere, kills one of them. Additional measurements remove clock error and atmospheric error.
Instructor setup: tape the Air Force One picture somewhere in the room and mark three fixed reference points as satellites 1, 2 and 3, then measure the distances with a tape before class and put the real numbers on this slide. The numbers shown are from the 2021 running of this activity: Satellite 1 = the light on the zoom camera, Satellite 2 = the light above row 2 left, Satellite 3 = the BYU sticker on the front control panel. For Clyde 254 the recorded set was 221 inches from the projector lens on the ceiling, 260 inches from the screw on the bottom of the front left speaker, and 149 inches from the angled smoke detector. Hand out tape measures and let them swing arcs. The point is that they will physically do what three spheres do.
This is the graded activity, worked on paper. Give them a printed map of Europe with a scale bar, or let them use a web map. Twelve to fifteen minutes. Circulate and check that they converted seconds to kilometers before drawing anything.
Check the arithmetic with them: 0.00237 s x 299,792 km/s = 710.5 km. The original speaker notes list 711, 885 and 1035 km, and label the first one "miles" by mistake; they are all kilometers.
Reveal only after they have committed to an answer. Ask what a fourth station would have added: a check on their own clock. Ask what would happen if all three stations were in a line.
Ask why they do not just add: because it would be extraordinarily unlucky for every source to be at its maximum, in the same direction, at the same instant. The root sum of squares is the standard way to combine independent uncertainties, and they have seen it in statics and in measurements courses.
Give them three minutes to redo it with the low values: sqrt(1.5^2 + 0.5^2 + 5^2 + 0.5^2 + 0.3^2 + 0.6^2) is about 5.3 m, times 1.5 is about 8 m. That spread, 8 m to 40 m, is the honest answer to "how accurate is GPS?"
Left: a single range is really a fuzzy band, because the measured time is uncertain. Right: two or more fuzzy bands intersect in a patch, not a point. The shape of that patch is set entirely by the angles between the satellites.
Same range uncertainty in both pictures. The only difference is where the satellites are. This is why your fix improves if you wait ten minutes, and why it is bad in a canyon: you only see the strip of sky overhead.
Answer B. Satellite count matters only up to a point; geometry is what multiplies your error. Five well-spread satellites beat seven clustered ones. This is why field receivers report PDOP and why survey planning software predicts it hours ahead.
Do the cosine live. Then ask the trap question: "what is the distance between 40.2500, -111.6500 and 40.2600, -111.6600?" If anyone answers using degrees, that is the lesson.
Run this live and let them follow along. If the network is down, the tagis site is the only online piece; the QGIS half works offline. This is the same workflow they need for Lab 3.
QGIS does apply an ellipsoidal correction when the project ellipsoid is set, so the measure tool may still give a sensible meter value in a geographic CRS. Show both, and make the point that the field calculator and most geoprocessing tools will not do that for you.
111,320 / 84,960 = 1.31, which is the signature of that particular mistake at this latitude. Worth naming so they recognize it in the lab.
Close the loop on the instrument-versus-user point from Tuesday. System and other flaws are under about 9 meters; user error can be plus or minus a kilometer. Everything in today's checklist is about the second number.
Confirm the Saturday due dates against Learning Suite before class. Remind them that Lab 3 uses the points they collected on Tuesday, so anyone who missed the activity needs to go collect three points.
Conversion notes (2026-09-02): sources were "GPS and Triangulation.pptx" (2025) slides 1-5, 13-15, 22, 24-26 and, for the four-step position-fixing build, "GPS basics.pptx" (2024) slides 33-36, a legacy Trimble real-time-surveying deck whose pale blue slide background was whitened when the figures were extracted. Hidden source slide 5 (the classroom distances for the Air Force One activity) was kept deliberately as an instructor backup: the three distances are on the activity slide and the 2021 satellite locations plus the Clyde 254 alternative are in its speaker notes — the instructor should re-measure for the actual room. Hidden slide 13 ("d1 d2 d3") was dropped as a bare shape overlay with no context. No ArcGIS screenshots appear in either source deck, so no QGIS re-shoots are needed; the QGIS workflow on the "Demo, step by step" and "Now measure something" slides was written for this deck. New material not in the sources, written to cover the assigned topics: the triangulation-versus-trilateration slide, the root-sum-of-squares error computation and its worked example, the PDOP quiz, and the whole latitude/longitude-to-meters demo section. The Prague distances are computed from the source delays and match the numbers in the original speaker notes; the original note labels the Amsterdam distance "miles", which is a typo for kilometers.