A measurement of the ({W}^{+}{W}^{-}) boson pair production cross section in proton-proton collisions at (\sqrt{s}=13\text{}\text{}\mathrm{TeV}) is presented. The data used in this study are collected with the CMS detector at the CERN LHC and correspond to an integrated luminosity of (35.9\text{}\text{}{\mathrm{fb}}^{-1}). The ({W}^{+}{W}^{-}) candidate events are selected by requiring two oppositely charged leptons (electrons or muons). Two methods for reducing background contributions are employed. In the first one, a sequence of requirements on kinematic quantities is applied allowing a measurement of the total production cross section, (117.6±6.8\text{}\text{}\mathrm{pb}), which agrees well with the theoretical prediction. Fiducial cross sections are also reported for events with zero or one jet, and the change in the zero-jet fiducial cross section with the jet transverse momentum threshold is measured. Normalized differential cross sections are reported within the fiducial region. A second method for suppressing background contributions employs two random forest classifiers. The analysis based on this method includes a measurement of the total production cross section and also a measurement of the normalized jet multiplicity distribution in ({W}^{+}{W}^{-}) events. Finally, a dilepton invariant mass distribution is used to probe for physics beyond the standard model in the context of an effective field theory, and constraints on the presence of dimension-6 operators are derived.