The observation of solar neutrinos by Kamiokande shows that the solar-neutrino problem cannot be solved by changing the solar model. In combination with the observations with a chlorine detector, it makes the nonadiabatic form of the Mikheyev-Smirnov-Wolfenstein theory most likely, and determines AmZsin20= 1.OX lo-' ev2. Probably all neutrinos go through the resonance in the Sun, those from 'B nonadiabatically, all others adiabatically. The latter emerge from the Sun in the higher-mass eigenstate vz and have a probability sin20 to be detected as v,. The gallium experiments, when done with sufficient accuracy, will be able to determine Am = m 2(v,) -m '(v, ) within fairly close limits. If the day-night effect can be measured, it will further constrain these limits. The small value of Am 2sin20 explains why the oscillation from v, to v, has not been observed in the laboratory. From existing experiments, the temperature at the center of the Sun can be determined to be within about 6% of that derived from the standard solar model; future neutrino experiments may determine it to within 1%.