Systems composed of 3 nucleons are a subject of precise experimental studies for many years. At the first stage the investigations were mainly focused on elastic nucleon-deuteron scattering, slowly extending to systematic measurements of the deuteron breakup reaction. Intermediate energies, below the threshold for pion production, deserve special attention: it is the region where comparison with exact theoretical calculations is possible, while the sensitivity to various aspects of interaction, like subtle effects of the dynamics beyond the pairwise nucleon-nucleon force, is significant. Moreover, the Coulomb interaction and relativistic effects show their influence in the observables of the breakup reaction. All these effects vary with energy and appear with different strength in certain observables and phase space regions, what calls for systematic investigations of a possibly rich set of observables determined in a wide range of energies. The next step in complication of the system are studies of reactions involving 4 nucleons-more sensitive, as expected, to subtle dynamics beyond the pairwise interaction. A brief survey of recent and planned experiments in the 3-and 4-nucleon systems is given.An important, and even basic step on the way to understand properties of nuclei and reactions involving nucleons and nuclei would be to create an exact model of nuclear forces. Even though from the QCD point of view nuclear forces are given as residual interaction between hadrons, successful calculations in the energy region of stable nuclei can be performed with just nuclear and pionic degrees of freedom. At present, there are generally two approaches to the construction of nucleon-nucleon potential: realistic potentials, which are semi-phenomenological models based on meson-exchange picture (see [1] for review), and effective field theories based on spontanously broken chiral symmetry (see [2,3] and references therein). They both provide an accurate description of the very large N N scattering data base below the pion production threshold. The modern potentials were tuned to these large data sets by means of PWA [4,5] and, as a result, the structure of the nuclear force in terms of angular momenta has been established. The nucleon-nucleon potential is undoubtedly a leading part of the nuclear interaction and should be sufficient to describe basic properties of nuclei and main trends in observables for systems of few (and many) nucleons, if only exact calculations are feasible. However, since an internal structure of nucleons is neglected, the question arises, how the suppressed degrees of freedom influence observables in any system consisting of more than 2 nucleons. Such additional dynamics, called