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In theory, the spring constant of an "ideal" spring can be found as k = E A 0 L 0, where E is the Young's modulus of the material, A 0 is the unstretched cross sectional area and L 0 is the unstretched length of the spring.
Fig. 2 Ideal spring characteristic for iso-elastic behaviour (ideal) compared to multiple real spring curves (a Art Nr. 22/2/2, b Art Nr. 22/8/2, c Art Nr. 25/4/3, d Art Nr. 25/5/2, e Art Nr. 26/4/1) Source: Durovis AG, Switzerland Fig. 3 Position ((varphi)) versus load (F_z) for different bar lengths b.
If \Delta x is the displacement, the force exerted by an ideal spring equals: :\vec{F}=-k \Delta \vec{x} where k is the spring constant (or force constant), which is particular to the spring.
The ideal spring starter, equally lovely as a refreshing lunch on a hot summer's day.
In this context, a diatomic molecule may be modeled as two masses connected by an ideal spring.
Simulations were performed in a broad temperature range and for intra-chain interactions varying from the fully interacting to the ideal spring chain.
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