We present a general study of oscillations in suspended one-dimensional elastic systems clamped at each end, exploring a wide range of slack (excess length) and downward external forces. Our results apply directly to recent experiments in nanotube and silicon nanowire oscillators. We find the behavior to simplify in three well-defined regimes which we present in a dimensionless phase diagram. The frequencies of vibration of such systems are found to be extremely sensitive to slack.Vibrations of one-dimensional systems (i.e. systems with cross-sectional dimension much smaller than their length) suspended under the influence of a downward force have long been of interest in the context of such applications as beams, cables supporting suspension bridges and ship moorings [1,2,3]. Such systems display a wide range of behavior, depending on the amount of slack present in the system, the downward force, and the aspect ratio. Previous studies, which have largely been analytical, have been restricted to certain limiting cases of these parameters. Recently work on oscillating nanoscale systems, such as carbon nanotubes [4] and silicon nanowires [5], has opened the possibility of experimentally exploring such vibrations in entirely new regimes. In the present work, we study numerically the oscillations of a one dimensional elastic system over an extensive range of both the slack and force parameters, providing insight into the physics which separates this parameter space into three distinct regimes of behavior.The treatment below is entirely general with illustrative examples taken from parameters relevant to carbon nanotubes. Since their discovery in 1991 [6], nanotubes have found many applications in device technology due to their small size, robust structure and superior elastic properties [7,8,9,10]. Many of these applications involve the use of nanotubes as mechanical oscillators, making theoretical understanding of the vibrational properties of nanotubes in various geometries of current interest [4,11]. Recent experiments [12] have studied the behavior of the transverse vibrations of a suspended nanotube clamped at both ends, under the action of a downward force, as sketched in Figure 1. These suspended nanotubes generally have around 1% slack, denoted in this work by s, which we define to be the ratio of the excess length of the tube to the distance between clamping points.Analytic model and computational techniques -The potential energy of a one-dimensional elastic continuum under a uniform downward force isHere, l represents distance along the system of unstretched length L; u(l), R(l) and z(l) represent the local strain, radius of curvature and vertical displacement, 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000111 111 respectively; E and F are the extensional and flexural rigidities; and f is the downward force per unit length. For single-walled nanotubes with diamet...