You could say that, but you'd be wrong. Most solid matter is not black at all. And you don't need something to be solid in order to be black.
The only blackbody that is not solid matter is the "sun", supposedly.
A blackbody spectrum is the property of solid matter, or pressure broadened plasma, approaching solid matter, here on earth in a lab.
You cannot get a blackbody in a thin plasma here on earth. I know this from my work with cavitation.
Uh... no. No, they don't. That's why they're called black bodies: because they don't reflect light. If they reflected light, they'd be the color of whatever light they reflected. If they reflect red light only, they would be red bodies. If they reflected blue light only, they would be blue bodies. If they reflect all light, they are white bodies.
No solid matter is black enough to absorb 100% of the incident light.
There is always some small percentage of reflected light.
"On the other hand, researchers now say they have created the darkest material ever made by man. The material, a thin carbon coating, reflects less than 0.1 percent of incoming light. It absorbs the rest."
http://www.world-science.net/othernews/080223_black.htm
You're half wrong. Emission is indeed one of the two ways to see a black body. The other way to see something black is via its silhouette. Reflection, however, is NOT one of the ways to see a black body. Because, once again, if it's a black body, it doesn't reflect light! That's what black body means. Once again, you're wrong by definition, which is about as wrong as you can possibly be.
See above.
Once again reality and the lab trump theory and "definition". This perfect blackbody only exists in theory. The sun actually has a hump in the EUV which makes it a "not perfect blackbody".
http://folk.uio.no/paalb/sumer_atlas.html
http://climate.gsfc.nasa.gov/static/cahalan/Radiation/Images/SolarIrrVblackbody.gif
From the JET website.
"The Science of JET", by John Wesson".
"The initial idea was that of detecting the blackbody radiation from the thermal plasma ions. However, when the ICE spectra were measured they were not consistent with this expectation, having instead narrow equally-spaced emission lines, the spacing being proportional to the magnetic field, and intensities much larger than the blackbody level. The spectrum from a deuterium-tritium plasma is shown in Figure 13.4 (below). The observed frequencies depend on the magnitude of the magnetic field at the location of the emission and, surprisingly, it was found that in JET this meant that the emission comes from the edge of the plasma in the outer midplane."
Canada's Ultimate Light Ruler
"The core of the high-temperature blackbody is a hollow tube of a special form of graphite that can withstand intense heating. In order to produce the required UV radiation, the graphite core is heated to approximately 3230 ºC, a temperature at which almost all metals melt – hence the name an ultra high-temperature blackbody. The graphite is gradually heated over the course of several hours in the same way a stove element is heated – by running an electrical current through it. The graphite core is insulated with many concentric layers of carbon cloth which are water-cooled.
At 3230 ºC any oxygen would react instantly with the graphite, causing a fire. So, during operation the entire core is flushed with argon, a non-reactive gas. At operating temperature, the high-temperature blackbody produces an intense beam of light that's emitted from a tiny eight millimetre hole – a beam of light that will soon be Canada's ultimate light ruler."
http://www.nrc-cnrc.gc.ca/eng/news/nrc/2006/02/06/black-body.html