mono_gauss_coil

Scattering from monodisperse polymer coils

Parameter	Description	Units	Default value
scale	Source intensity	None	1
background	Source background	cm-1	0.001
i_zero	Intensity at q=0	cm-1	70
rg	Radius of gyration	Å	75

The returned value is scaled to units of cm^-1 sr^-1, absolute scale.

This Debye Gaussian coil model strictly describes the scattering from monodisperse polymer chains in theta solvents or polymer melts, conditions under which the distances between segments follow a Gaussian distribution. Provided the number of segments is large (ie, high molecular weight polymers) the single-chain form factor P(Q) is that described by Debye (1947).

To describe the scattering from polydisperse polymer chains see the poly_gauss_coil model.

Definition

$$I(q) = \text{scale} \cdot I_0 \cdot P(q) + \text{background}$$

where

$$\begin{split}I_0 &= \phi_\text{poly} \cdot V \cdot (\rho_\text{poly} - \rho_\text{solv})^2 \\ P(q) &= 2 [\exp(-Z) + Z - 1] / Z^2 \\ Z &= (q R_g)^2 \\ V &= M / (N_A \delta)\end{split}$$

Here, $\phi_\text{poly}$ is the volume fraction of polymer, $V$ is the volume of a polymer coil, M is the molecular weight of the polymer, $N_A$ is Avogadro’s Number, $\delta$ is the bulk density of the polymer, $\rho_\text{poly}$ is the sld of the polymer, $\rho\text{solv}$ is the sld of the solvent, and $R_g$ is the radius of gyration of the polymer coil.

The 2D scattering intensity is calculated in the same way as the 1D, but where the q vector is redefined as

$$q = \sqrt{q_x^2 + q_y^2}$$

Fig. 109 1D plot corresponding to the default parameters of the model.

References

P Debye, J. Phys. Colloid. Chem., 51 (1947) 18.

R J Roe, Methods of X-Ray and Neutron Scattering in Polymer Science, Oxford University Press, New York (2000).

http://www.ncnr.nist.gov/staff/hammouda/distance_learning/chapter_28.pdf