Axially flexible bar or cable

**Library:**Simscape / Driveline / Couplings & Drives

The Rod block represents an axially flexible bar or cable in tension or compression.

To represent the bar or cable, the block uses a lumped parameter model. The model is
composed of *N*+1 lumped masses that are connected in series by *N*
sets of parallel-connected spring and damper circuits. The spring represents
elasticity. The damper represents material damping.

A single segment model exhibits an eigenfrequency that is close to the first eigenfrequency of the distributed parameter model. For more accurate analysis, select 2, 4, 8, or more segments.

The equivalent physical network contains *N* spring and damper circuits
and *N*+1 mass blocks. The total mass of the rod is distributed evenly over
the mass blocks. The stiffness of the spring in each spring and damper circuit is
equal to the *N* times the stiffness of the rod
material.

The defining equations for the model are:

$$\eta =2\zeta \sqrt{\frac{K\cdot m}{2}}$$

$$A=\frac{\pi ({D}^{2}-{d}^{2})}{4}$$

$$K=\frac{E\cdot A}{L}$$

$$m=A\cdot L\cdot \rho $$

Where:

*η*is the damping of the rod.*ς*is the damping ratio of the rod material.*K*is the stiffness of the rod.*A*is the cross-sectional area of the rod.*D*is the outer diameter of the rod.*d*is the inner diameter of the rod, where*d*= 0 for a solid rod.*d*> 0 for an annular, that is, hollow, rod.

*E*is Young's modulus, that is, the modulus of elasticity, of the rod material.*L*is the length of the rod.*m*is the mass of the rod.*ρ*is the density of the rod material.

The rod does not buckle, in the case of a bar, or go slack, in the case of a cable, in tension.

The rod has a constant cross-section along its length.

The distributed parameter model is approximated as a finite number of segments,

*N*.

Flexible Shaft | Mass | Translational Damper | `Translational Spring`