Retain spectral convention before inferring a temperature
An ideal blackbody continuum is a useful physical reference, not a universal description of every astronomical source. Its temperature controls both shape and emitted power. The Planck function Bλ=2hc²/[λ⁵(exp(hc/(λkT))−1)] describes spectral radiance per unit wavelength and solid angle. The subscript matters: Bν per frequency is a different density representation of the same radiation.
Learning outcome: Compare temperature at a fixed selected wavelength. Retain Bλ units, peak, color ratio and integrated surface flux; explain why a normalized shape and one observed color do not uniquely determine a real source.
Starting recap
Keep photon energy/count, density convention, propagation, collection/resolution, calibration and source-quality assumptions distinct.
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At 6000 K, the Bλ peak is≈482.962 nm and Bλ(400)/Bλ(800)≈1.52132. Ideal surface flux is≈7.34881×10^7 W/m². A 3000 K blackbody peaks near 965.924 nm and has ratio≈0.0795272; its normalized plot can still reach one despite much lower absolute emission.
Open the experimentPredict
If two plotted curves are each normalized to a peak of one, does that establish equal emitted power?
Experiment
Compare temperature at a fixed selected wavelength. Retain Bλ units, peak, color ratio and integrated surface flux; explain why a normalized shape and one observed color do not uniquely determine a real source.
Keep spectral-density convention in a thermal color comparison
Worked teaching model · synthetic values · Ideal Planck B_lambda per meter per steradian, not B_nu; wavelength peak b/T with b=2.897771955e−3 m K. Color ratio uses 400/800 nm B_lambda; no dust, line blanketing or real stellar atmosphere fit. Curve normalized to B_lambda peak.
Reset keeps your prediction, captures and practice history.
A thermal color or peak requires a spectral-density convention and a physical emission model.
The same radiation plotted per frequency has a different peak coordinate. Normalizing the curve removes its absolute flux information; dust, spectral lines and detector bandpasses complicate an actual temperature inference.
| Vacuum wavelength / nm | B_lambda / peak B_lambda |
|---|---|
| 100 | 0.00001440892 |
| 120 | 0.0003150849 |
| 140 | 0.002532101 |
| 160 | 0.01104999 |
| 180 | 0.03241972 |
| 200 | 0.07254229 |
| 220 | 0.1339697 |
| 240 | 0.2150569 |
| 260 | 0.3108528 |
| 280 | 0.4147403 |
| 300 | 0.5199737 |
| 320 | 0.6207199 |
| 340 | 0.7125621 |
| 360 | 0.7925964 |
| 380 | 0.8592805 |
| 400 | 0.9121695 |
| 420 | 0.9516261 |
| 440 | 0.9785556 |
| 460 | 0.9941876 |
| 480 | 0.9999085 |
| 500 | 0.9971408 |
| 520 | 0.9872628 |
| 540 | 0.9715577 |
| 560 | 0.9511864 |
| 580 | 0.9271751 |
| 600 | 0.9004152 |
| 620 | 0.8716683 |
| 640 | 0.8415771 |
| 660 | 0.8106761 |
| 680 | 0.7794053 |
| 700 | 0.7481215 |
| 720 | 0.7171108 |
| 740 | 0.6865986 |
| 760 | 0.6567594 |
| 780 | 0.6277251 |
| 800 | 0.5995924 |
| 820 | 0.5724288 |
| 840 | 0.5462781 |
| 860 | 0.5211649 |
| 880 | 0.4970985 |
| 900 | 0.4740757 |
| 920 | 0.4520840 |
| 940 | 0.4311032 |
| 960 | 0.4111078 |
| 980 | 0.3920678 |
| 1000 | 0.3739505 |
| 1020 | 0.3567212 |
| 1040 | 0.3403441 |
| 1060 | 0.3247825 |
| 1080 | 0.3100002 |
| 1100 | 0.2959608 |
| 1120 | 0.2826289 |
| 1140 | 0.2699697 |
| 1160 | 0.2579497 |
| 1180 | 0.2465362 |
| 1200 | 0.2356981 |
| 1220 | 0.2254054 |
| 1240 | 0.2156294 |
| 1260 | 0.2063427 |
| 1280 | 0.1975192 |
| 1300 | 0.1891343 |
| 1320 | 0.1811643 |
| 1340 | 0.1735870 |
| 1360 | 0.1663813 |
| 1380 | 0.1595271 |
| 1400 | 0.1530055 |
| 1420 | 0.1467988 |
| 1440 | 0.1408899 |
| 1460 | 0.1352629 |
| 1480 | 0.1299028 |
| 1500 | 0.1247954 |
| 1520 | 0.1199273 |
| 1540 | 0.1152858 |
| 1560 | 0.1108590 |
| 1580 | 0.1066355 |
| 1600 | 0.1026049 |
| 1620 | 0.09875709 |
| 1640 | 0.09508258 |
| 1660 | 0.09157247 |
| 1680 | 0.08821834 |
| 1700 | 0.08501225 |
| 1720 | 0.08194669 |
| 1740 | 0.07901458 |
| 1760 | 0.07620924 |
| 1780 | 0.07352435 |
| 1800 | 0.07095393 |
| 1820 | 0.06849236 |
| 1840 | 0.06613429 |
| 1860 | 0.06387470 |
| 1880 | 0.06170882 |
| 1900 | 0.05963213 |
| 1920 | 0.05764038 |
| 1940 | 0.05572953 |
| 1960 | 0.05389575 |
| 1980 | 0.05213544 |
| 2000 | 0.05044516 |
| Quantity | Value | Unit |
|---|---|---|
| B_lambda peak wavelength | 482.9620 | nm |
| Selected spectral radiance B_lambda | 2.867639e+13 | W m⁻² sr⁻¹ m⁻¹ |
| 400/800 nm B_lambda ratio | 1.521316 | ratio |
| Integrated ideal surface flux | 7.348805e+7 | W/m² |
| Selected/peak B_lambda | 0.9004152 | ratio |
Actual SDSS records are explicitly labeled; all other packets are original models. No direct solar viewing, radiation experiment or instrument operation is requested.
A thermal color or peak requires a spectral-density convention and a physical emission model.
The same radiation plotted per frequency has a different peak coordinate. Normalizing the curve removes its absolute flux information; dust, spectral lines and detector bandpasses complicate an actual temperature inference.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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Public practice checks a specific claim. It does not establish independent mastery.
Double temperature from 3000 to 6000 K. What happens to the wavelength peak and integrated ideal surface flux?
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