We focus on the fact that light-pulse atom interferometers measure the atoms' acceleration with only 3 data points per drop. As a result the measured effect of gravity gradient is systematically larger than the real one, an error almost unnoticed so far. We show how it affects the absolute measurement of the gravitational acceleration g as well as ground and space experiments based on gradiometers such as those designed for space geodesy, the measurement of the universal constant of gravity and the detection of gravitational waves. Tests of the weak equivalence principle need two different atom species. If both species can be operated with the same laser the error reported here cancels out. If not, the fractional differences in pulse timing and momentum transfer set the precision of the test at unacceptable levels and severely limit the atoms' choice, whereby most tests use isotopes of the same Rb atom which differ by two neutrons only.Light-pulse Atom Interferometers (AIs) are based on quantum mechanics. As the atoms fall, the atomic wave packet is split, redirected, and finally recombined via three atom-light interactions at times 0, T , 2T . The phase that the atoms acquire during the interferometer sequence is proportional to the gravitational acceleration that they are subjected to.It has been shown ([1], Sec. 2.1.3) that although one might think that the phase shift depends on quantum mechanical quantities ". . . this is merely an illusion since we can write the scale factor [between the phase shift and the gravitational acceleration] in terms of the parameters we control experimentally, i.e. Raman pulse vector k and pulse timing T . It then takes the form kT 2 . . . . We can simply ignore the quantum nature of the atom and model it as a classical point particle that carries an internal clock and can measure the local phase of the light field." In the same reference it is demonstrated that both the exact path integral approach and the purely classical one lead to the same exact closed form for the phase shift and free fall acceleration measured by the AI, which is then expanded in power series of the local gravity gradient γ for convenience [1]. The only remaining sign of the atom-light interaction -which cannot possibly appear in the classical model where there is no such interactionis the recoil velocity. However, it neither appears in the phase shift actually measured by AIs because they are operated symmetrically so as to cancel it out (or make it smaller than the initial velocity errors) [2,3]. Thus, the classical approach gives excellent predictions of the phase shift measured by the interferometer, while including the quantum mechanical details related to the internal degrees of freedom is needed to account for smaller effects, such as the finite length of the light pulses.We focus on the fact that AIs measure the atoms position along the trajectory only 3 times per drop (in correspondence of the 3 light pulses), unlike laser interferom-eters in falling corner-cube gravimeters which make hundreds to ...