- Timestamp:
- Oct 28, 2017 4:02:56 AM (7 years ago)
- Branches:
- master, core_shell_microgels, magnetic_model, ticket-1257-vesicle-product, ticket_1156, ticket_1265_superball, ticket_822_more_unit_tests
- Children:
- 75e4319
- Parents:
- 6db17bd
- Location:
- doc/guide/pd
- Files:
-
- 1 added
- 1 edited
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doc/guide/pd/polydispersity.rst
r1f058ea ra5a12ca 40 40 calculations are generally more robust with more data points or more angles. 41 41 42 The following fivedistribution functions are provided:42 The following six distribution functions are provided: 43 43 44 44 * *Rectangular Distribution* … … 47 47 * *Schulz Distribution* 48 48 * *Array Distribution* 49 * *Boltzmann Distribution* 49 50 50 51 These are all implemented as *number-average* distributions. … … 181 182 ^^^^^^^^^^^^^^^^^^ 182 183 183 This user-definable distribution should be given as a s asimple ASCII text184 This user-definable distribution should be given as a simple ASCII text 184 185 file where the array is defined by two columns of numbers: $x$ and $f(x)$. 185 186 The $f(x)$ will be normalized to 1 during the computation. … … 200 201 given for the model will have no affect, and will be ignored when computing 201 202 the average. This means that any parameter with an array distribution will 202 not be fittable. 203 not be fitable. 204 205 .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ 206 207 Boltzmann Distribution 208 ^^^^^^^^^^^^^^^^^^^^^^ 209 210 The Boltzmann Distribution is defined as 211 212 .. math:: 213 214 f(x) = \frac{1}{\text{Norm}} 215 \exp\left(-\frac{ | x - \bar x | }{\sigma}\right) 216 217 where $\bar x$ is the mean of the distribution and *Norm* is a normalization 218 factor which is determined during the numerical calculation. 219 The width is defined as 220 221 .. math:: \sigma=\frac{k T}{E} 222 223 which is the inverse Boltzmann factor, 224 where $k$ is the Boltzmann constant, $T$ the temperature in Kelvin and $E$ a 225 characteristic energy per particle. 226 227 .. figure:: pd_boltzmann.jpg 228 229 Boltzmann distribution. 203 230 204 231 .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
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