SIXMILE RUN

TARGET 10 · l = 0°, b = 90° · Coma Berenices

North Galactic Pole

Straight up out of the disk, through the least hydrogen you can find in the northern sky. The off-plane comparison every on-plane spectrum needs.

RA / Dec (J2000)
12h 51m 26s
+27.1°
Transits at midnight
5 Apr
local mean time
Model vLSR range
n/a
off the plane
LSR correction over a year
−18 to +34
km/s at 40° N, 75° W

Not every useful pointing is a bright one.

Why point here. Looking straight out of the Galactic disk, the path length through hydrogen is as short as it gets, so the line is far weaker than anywhere in the plane. Weak is not zero: there is still local gas above and below the Sun. That makes the pole a useful comparison. A spectrum that looks just as strong here as it does in Cygnus is telling you something about your bandpass correction or about local interference, not about the sky.

What you’ll see. A faint line near zero velocity, or nothing at all with a small antenna and a short integration. Use the radiometer equation to work out how long you would need to integrate to see it, then decide whether that’s worth the time. Often the better use is a quick comparison: take the same integration here and in the plane, and check that the difference between them looks like a line.

No velocity model. The rotation model on the other target pages only describes gas in the plane. At b = 90° it doesn’t apply, so this page doesn’t show one.

Practicalities. At +27° declination it rises well from both hemispheres, culminating near 77° from 40° N. It transits at midnight in early April. The South Galactic Pole, in Sculptor, does the same job for southern observers.

How high it gets

Altitude at meridian transit and time above the horizon per sidereal day, for this pointing at a range of observer latitudes. Below about 20° the beam starts picking up ground, so the last column is the one to plan on.

LatitudeTransit altitudeAbove horizonAbove 20°
60° N57°20.3 h12.9 h
50° N67°17.0 h12.1 h
40° N77°15.4 h11.4 h
30° N87°14.3 h10.8 h
20° N83°13.4 h10.3 h
0°63°12.0 h9.0 h
20° S43°10.5 h7.1 h
35° S28°9.2 h4.5 h

Transit time by month

Local mean time of meridian transit on the 1st of each month. That is clock time without daylight saving, corrected by four minutes for every degree you sit east or west of your time zone's central meridian. The tools do it for your exact site. The transit comes about four minutes earlier each day.

  1. Jan06:09
  2. Feb04:07
  3. Mar02:17
  4. Apr00:15
  5. May22:13
  6. Jun20:11
  7. Jul18:13
  8. Aug16:11
  9. Sep14:09
  10. Oct12:11
  11. Nov10:10
  12. Dec08:12

Read alongside

Coordinates, visibility, transit times and the LSR swing are computed for this page with the same code as our calculators. The velocity model is circular rotation on a flat curve with R₀ = 8.5 kpc and V₀ = 220 km/s (IAU 1985), the textbook first approximation. Real spectra depart from it, and the notes above say where. Found an error? Tell us.