In this paper, we assess the validity of a universal solution based on the slenderness approximation to describe the velocity and shape of viscous capillary jets produced by two very different mechanisms: the action of the constant gravity force and the focusing effect of a coflowing gas stream. In the gravitational case, the jet's velocity distribution given by the universal solution is compared with that calculated numerically from the Navier-Stokes equations. The universal solution provides remarkably good predictions for the wide range of parameters considered in this work. Its accuracy generally improves as the Reynolds number increases and/or the Froude number decreases, probably because the jet viscous region decreases in this case. The flow focusing method was examined experimentally by acquiring and processing images of the tapering liquid meniscus formed between the feeding capillary and the discharge orifice. In this case, the universal solution provides satisfactory results for sufficiently slender liquid meniscus (i.e., for sufficiently large liquid viscosities and flow rates and small applied pressure drops), provided that the ratio capillaryto-orifice distance H to orifice diameter D takes sufficiently small values. If these conditions are not satisfied, the universal solution underestimates the jet radius close to the feeding capillary, but it still provides accurate predictions beyond the discharge orifice. For small H/D values, the accuracy of the universal solution is mainly limited by radial momentum effects associated with the sharp contraction of the meniscus shape, which becomes less slender as the liquid viscosity and flow rate decrease, or the pressure drop increases. For large H/D values, the driving force significantly deviates from its assumed constant value in the universal solution, giving rise to larger discrepancies between that solution and the experimental results even for slender shapes.