Question

A rubber band is composed of a \"bundle\" of polymers, which form very long linear molecules or chains of simpler molecular units called monomers. These molecules can coil or unfold depending on the temperature and applied tension, giving these systems their elastic properties. The simplest equations of state for a system like this are given by: $U = cL_0T$ (5) $\tau = bT\frac{L - L_0}{L_1 - L_0}$ (6) Where $c$ and $b$ are constants, $\tau$ represents the tension applied to the band at its elastic limit, $L_0$ is the length of the unstretched band, and $L_1$ represents the limit length of the band to which it can stretch without losing its elastic properties. From equations (5) and (6), obtain the fundamental relationship of the rubber band.

          A rubber band is composed of a \"bundle\" of polymers, which form very long linear molecules or
chains of simpler molecular units called monomers. These molecules can coil or unfold depending
on the temperature and applied tension, giving these systems their elastic properties. The
simplest equations of state for a system like this are given by:
$U = cL_0T$ (5)
$\tau = bT\frac{L - L_0}{L_1 - L_0}$ (6)
Where $c$ and $b$ are constants, $\tau$ represents the tension applied to the band at its elastic limit, $L_0$ is
the length of the unstretched band, and $L_1$ represents the limit length of the band to which it can
stretch without losing its elastic properties.
From equations (5) and (6), obtain the fundamental relationship of the rubber band.

A rubber band is composed of a b̈undleöf polymers, which form very long linear molecules or
chains of simpler molecular units called monomers. These molecules can coil or unfold depending
on the temperature and applied tension, giving these systems their elastic properties. The
simplest equations of state for a system like this are given by:
U = cL0T (5)
τ = bT(L - L0)/(L1 - L0) (6)
Where c and b are constants, τ represents the tension applied to the band at its elastic limit, L0 is
the length of the unstretched band, and L1 represents the limit length of the band to which it can
stretch without losing its elastic properties.
From equations (5) and (6), obtain the fundamental relationship of the rubber band.

Added by Brenda F.

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