Thin, solid bodies with metric symmetries admit a restricted form of reparameterization invariance. Their dynamical equilibria include motions with both rigid and flowing aspects. On such configurations, a quantity is conserved along the intrinsic coordinate corresponding to the symmetry. As an example of its utility, this conserved quantity is combined with linear and angular momentum currents to construct solutions for the equilibria of a rotating, flowing string, for which it is akin to Bernoulli's constant.The mechanics of thin bodies are amenable to a description in which energies are effectively expressed with an integral over a surface or curve. On sufficiently long time scales, and when longitudinal waves are not important, the effective action is often taken to be metrically constrained, with a low-dimensional body stress tensor enforcing local distances between moving pieces of material. This approach, either at the level of the action or equations of motion, has been used to describe systems at many scales, from the overdamped motions of flagella [1,2] Thin bodies such as rods and solid membranes moving in a higher-dimensional space share characteristics with both rigid bodies and fluids. The metric constraints of inextensible solids preclude the broad reparameterization invariance inherent to fluids and fluid membranes, leaving only highly restricted reparameterization invariance associated with any metric symmetries the body may possess. Effectively one has global, rather than local, symmetries on the body. However, these intrinsic symmetries are not trivially identifiable with rigid transformations of embedding coordinates, because a lower-dimensional body can adopt extrinsic curvature in the surrounding space. Thus, unlike space-filling rigid continua, the body may display additional material flows in equilibrium in addition to, and distinct from, rigid motions. Simple examples include a string being unspooled [12], a cable being laid down on the ocean floor [14], or the flowing skirt of a rotating dancer [17]. Figure 1 is a schematic of such a combined rigid-flowing configuration.We will describe such a system using several types of coordinates. Aside from a time coordinate, there are three important sets of spatial coordinates to consider. First, there are time-independent coordinates attached to pieces of material. For an inextensible body, these can also be associated with geometric parameters, such as arc length. Second, there are coordinates for which material motions tangent to the body have been removed. These are effectively Eulerian from the intrinsic viewpoint of the body, but they are attached to a body moving through an embedding space, so have some Lagrangian character as well. This viewpoint is called the "orthogonal gauge" in [18]