russ_watters said:
Put a lid on the bucket and pump out the air. It will then be a water/vapor mixture at 100C and atmospheric pressure.
It will be somewhere on the liquid/vapor boundary, but would be colder than 100C, and lower than atmospheric pressure.
For the pure chemical case (e.g. water, with no air), it might help to see the 3D phase diagram, as shown here:
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/pvtexp.html#c1
We see that there is a 2D surface which you can regard as pressure as a function of temperature and volume. The state of the chemical is given by a point sitting somewhere along this surface. The surface is broken up into several faces which correspond to different phases. The formulae for the faces are called equations of state. (For example, the ideal gas law PV=nRT is an equation of state which is approximately valid in the "gas" part of the diagram above the critical temperature.)
If you put water in a closed container, this will constrain the density and volume, and the state will lie somewhere along the 2D cross section which looks like a traditional P vs T phase diagram. If the volume is large, that means your density is low, and you have only gas. If we half fill a bucket of water and pump out the remaining air, we will end up somewhere on the "liquid and vapor" face. That means there is an equilibrium between the liquid water, and the water vapor in the container. The pressure will be the vapor pressure of the chemical at whatever temperature it ends up at.
Therefore, it will be at the boiling "point", but as we can see on the 3D diagram, boiling is possible over a whole face (the liquid and vapor face), not a point.
In a closed container, we can't really control the pressure, unless we have some kind of piston.