The compressibility of calcite to 40 kbar has been remeasured by using a piston-cylinder apparatus. Calcite 1 is found to transform to calcite 2 at 14.5 kbar with a volume change of 0.00483 cmS/g, and calcite 2 is found to change to calcite 3 at 17.4 kbar with a volume change of0.012% cmS/g. The volume compression data for the three phases are described by the following quadratic relations: Calcite 1 --(AV/Vo) = -14.07 x lO-.P + 5.107 x lO-6P , Calcite 2 --(AV/Vo) = 0.where P is pressure in kilobars. The compression data for calcite 1 and calcite 3 are in good agreement with those available in the literature. The data exhibiting an abnormally high compression of calcite 2 have been reported for the first time. The compression data for calcite 2 have been used to explain quantitatively the abnormal drop near 15 kbar observed in the ultrasonic sound velocity in calcite. Bridgman [1939] observed that the atmospheric pressure phase of calcite (calcite l) transforms to calcite 2 near 15 kbar, and calcite 2 transforms to calcite 3 near 18 kbar. The compressibility of calcite 3 is abnormal in that it is higher than that of calcite I in spite of the fact that calcite 3 is the denser phase. Adaduroo et al. [1961] studied the compressibility of marble to 30 kbar by using a piston displacement piezometer and to 500 kbar by using shock compression and reported another transition at 11 kbar in addition to the two transitions reported by Bridgman [1939]. In a recent study, Vaidya et al. [1973] obtained compressibility data very similar to those of Bridgman [1939]; the two transitions, however, were not resolved in their experiments. The compressibility of calcite 2 could not be measured in many earlier studies because it exists over a small pressure range [Bridgman, 1939], and often the two transitions are not resolved [Bridgman, 1948; Vaidya et aL, 1973]. Besides a very rough estimate by Wang [1968], the only work reporting the compression of calcite 2 is by ,,ldaduroo et al. [1961]. The interest in the compressibility of calcite 2 stems from the fact that the ultrasonic sound velocity in calcite, limestones, and marbles exhibits a large decrease near 15 kbar [Wang, 1966]. In a further study, Wang [1968] showed that this drop is associated with the calcite l-calcite 2 transition and suggested a mechanism based on the oscillations of the domain boundaries between the two phases caused by ultrasonic waves to explain this drop. Using similar concepts, Walsh [1973] recently discussed the propagation of the ultrasonic waves in rocks undergoing polymorphic transformations. As was pointed out by Walsh [1973], this suggestion has much wider implications in the interpretations of the changes observed in the ultrasonic wave velocities. To understand the nature of the anomaly in calcite, a careful measurement of the compressibilities of calcite I and calcite 2 near the calcite l-calcite