Ion acoustic shocks are formed in a plasma with negative ions, where T
-e greater than or equal to T+ much greater than T- (T-e, T+, T-: temp
eratures of electrons, positive ions, and negative ions, respectively)
. Depending on the ratio epsilon of negative to positive density, a st
eepening of positive or negative density jumps is observed. For epsilo
n < epsilon(c) (approximate to 0.65, critical value), positive density
jumps evolve into compressive shocks. For epsilon > epsilon(c), howev
er, negative density jumps evolve into rarefactive shocks. The ratio e
psilon(c) observed is well explained on the basis of Korteweg-de Vries
equation.