Setting up the experimental design


We wanted to evaluate the effects of three thickeners of a generic ice cream mix on the viscosity of the mix and on the overrun of the finished ice cream, two parameters that influences in an important way the characteristics of the finished product.

We examined three thickeners commonly used as food additives:

We set up a mixture design of the Simplex Lattice type with k=3 and m=3, whose possible combinations led to carrying out 10 experimental conditions. We performed 3 replicates in 3 different weeks, although for this analysis we chose to consider only the last two sets of replicates..



df = read.csv("AddensantiDOE.csv", sep = ";")
week = rep(c(1,2,3), each=10 ) %>% factor()
df = add_column(df, Week = week, .after = "ID")


kable(df, row.names = T) %>% kable_styling('striped', fixed_thead = T, full_width = FALSE) %>%
  scroll_box( height = "500px")
ID Week FSC TARA GUAR Viscosity_cP Overrun
1 4_0_8 1 0.3333 0.0000 0.6667 4760 0.4845
2 4_4_4 1 0.3333 0.3333 0.3333 8750 0.3459
3 0_12_0 1 0.0000 1.0000 0.0000 9900 0.3039
4 0_8_4 1 0.0000 0.6667 0.3333 9800 0.2744
5 12_0_0 1 1.0000 0.0000 0.0000 6500 0.3690
6 8_0_4 1 0.6667 0.0000 0.3333 7400 0.3447
7 4_8_0 1 0.3333 0.6667 0.0000 9910 0.3163
8 0_0_12 1 0.0000 0.0000 1.0000 5480 0.5092
9 0_4_8 1 0.0000 0.3333 0.6667 5750 0.4532
10 8_4_0 1 0.6667 0.3333 0.0000 8990 0.3372
11 8_0_4 2 0.6667 0.0000 0.3333 7050 0.3572
12 0_8_4 2 0.0000 0.6667 0.3333 7200 0.4339
13 0_4_8 2 0.0000 0.3333 0.6667 6810 0.5000
14 4_8_0 2 0.3333 0.6667 0.0000 8370 0.3800
15 4_4_4 2 0.3333 0.3333 0.3333 7080 0.3968
16 0_0_12 2 0.0000 0.0000 1.0000 5790 0.5429
17 4_0_8 2 0.3333 0.0000 0.6667 6330 0.4619
18 0_12_0 2 0.0000 1.0000 0.0000 9330 0.2734
19 8_4_0 2 0.6667 0.3333 0.0000 7950 0.3647
20 12_0_0 2 1.0000 0.0000 0.0000 6330 0.3572
21 0_0_12 3 0.0000 0.0000 1.0000 4272 0.5653
22 8_4_0 3 0.6667 0.3333 0.0000 6780 0.3800
23 0_8_4 3 0.0000 0.6667 0.3333 5610 0.4935
24 4_8_0 3 0.3333 0.6667 0.0000 7500 0.3911
25 4_4_4 3 0.3333 0.3333 0.3333 6510 0.3968
26 12_0_0 3 1.0000 0.0000 0.0000 5730 0.3403
27 0_12_0 3 0.0000 1.0000 0.0000 8130 0.3498
28 4_0_8 3 0.3333 0.0000 0.6667 6450 0.5185
29 0_4_8 3 0.0000 0.3333 0.6667 5610 0.4496
30 8_0_4 3 0.6667 0.0000 0.3333 5610 0.4082


Postuleted model


Once the experiments have been carried out the data can be processed according to a simplified Scheffè model (special cubic), which allows to take into account the effects given by the possible interactions between the 3 variables FSC, TARA and GUAR.

The model is as follows:

\[ Y = b_0+b_1x_1+b_2x_2+b_3x_3+b_{12}x_1x_2+b_{13}x_1x_3+b_{23}x_2x_3+b_{123}x_1x_2x_3 \]

Additional columns related to 2-components interaction and 3-component interaction are then added to the starting dataset.

ID Week FSC TARA GUAR F_T T_G F_G F_T_G Viscosity_cP Overrun
1 4_0_8 1 0.3333 0.0000 0.6667 0.0000 0.0000 0.2222 0.000 4760 0.4845
2 4_4_4 1 0.3333 0.3333 0.3333 0.1111 0.1111 0.1111 0.037 8750 0.3459
3 0_12_0 1 0.0000 1.0000 0.0000 0.0000 0.0000 0.0000 0.000 9900 0.3039
4 0_8_4 1 0.0000 0.6667 0.3333 0.0000 0.2222 0.0000 0.000 9800 0.2744
5 12_0_0 1 1.0000 0.0000 0.0000 0.0000 0.0000 0.0000 0.000 6500 0.3690
6 8_0_4 1 0.6667 0.0000 0.3333 0.0000 0.0000 0.2222 0.000 7400 0.3447
7 4_8_0 1 0.3333 0.6667 0.0000 0.2222 0.0000 0.0000 0.000 9910 0.3163
8 0_0_12 1 0.0000 0.0000 1.0000 0.0000 0.0000 0.0000 0.000 5480 0.5092
9 0_4_8 1 0.0000 0.3333 0.6667 0.0000 0.2222 0.0000 0.000 5750 0.4532
10 8_4_0 1 0.6667 0.3333 0.0000 0.2222 0.0000 0.0000 0.000 8990 0.3372
11 8_0_4 2 0.6667 0.0000 0.3333 0.0000 0.0000 0.2222 0.000 7050 0.3572
12 0_8_4 2 0.0000 0.6667 0.3333 0.0000 0.2222 0.0000 0.000 7200 0.4339
13 0_4_8 2 0.0000 0.3333 0.6667 0.0000 0.2222 0.0000 0.000 6810 0.5000
14 4_8_0 2 0.3333 0.6667 0.0000 0.2222 0.0000 0.0000 0.000 8370 0.3800
15 4_4_4 2 0.3333 0.3333 0.3333 0.1111 0.1111 0.1111 0.037 7080 0.3968
16 0_0_12 2 0.0000 0.0000 1.0000 0.0000 0.0000 0.0000 0.000 5790 0.5429
17 4_0_8 2 0.3333 0.0000 0.6667 0.0000 0.0000 0.2222 0.000 6330 0.4619
18 0_12_0 2 0.0000 1.0000 0.0000 0.0000 0.0000 0.0000 0.000 9330 0.2734
19 8_4_0 2 0.6667 0.3333 0.0000 0.2222 0.0000 0.0000 0.000 7950 0.3647
20 12_0_0 2 1.0000 0.0000 0.0000 0.0000 0.0000 0.0000 0.000 6330 0.3572
21 0_0_12 3 0.0000 0.0000 1.0000 0.0000 0.0000 0.0000 0.000 4272 0.5653
22 8_4_0 3 0.6667 0.3333 0.0000 0.2222 0.0000 0.0000 0.000 6780 0.3800
23 0_8_4 3 0.0000 0.6667 0.3333 0.0000 0.2222 0.0000 0.000 5610 0.4935
24 4_8_0 3 0.3333 0.6667 0.0000 0.2222 0.0000 0.0000 0.000 7500 0.3911
25 4_4_4 3 0.3333 0.3333 0.3333 0.1111 0.1111 0.1111 0.037 6510 0.3968
26 12_0_0 3 1.0000 0.0000 0.0000 0.0000 0.0000 0.0000 0.000 5730 0.3403
27 0_12_0 3 0.0000 1.0000 0.0000 0.0000 0.0000 0.0000 0.000 8130 0.3498
28 4_0_8 3 0.3333 0.0000 0.6667 0.0000 0.0000 0.2222 0.000 6450 0.5185
29 0_4_8 3 0.0000 0.3333 0.6667 0.0000 0.2222 0.0000 0.000 5610 0.4496
30 8_0_4 3 0.6667 0.0000 0.3333 0.0000 0.0000 0.2222 0.000 5610 0.4082

Viscosity


Regression

A regression is made to find the optimal coefficients according to the model, evaluating their significance (95% confidence limit).

Being a model relative to a ternary mixture I don’t have the value relative to the intercept as for a traditional linear regression.



model = lm(Viscosity_cP~ 0+FSC+TARA+GUAR+F_T+F_G+T_G+F_T_G, df_complete)
summary(model)
## 
## Call:
## lm(formula = Viscosity_cP ~ 0 + FSC + TARA + GUAR + F_T + F_G + 
##     T_G + F_T_G, data = df_complete)
## 
## Residuals:
##      Min       1Q   Median       3Q      Max 
## -1856.37  -752.17    98.34   657.45  2333.63 
## 
## Coefficients:
##       Estimate Std. Error t value Pr(>|t|)    
## FSC     6300.4      575.3  10.952 1.34e-10 ***
## TARA    9102.2      575.3  15.822 7.44e-14 ***
## GUAR    5084.8      575.3   8.839 7.44e-09 ***
## F_T     2469.3     2689.2   0.918    0.368    
## F_G     2583.5     2689.2   0.961    0.347    
## T_G    -1335.7     2689.2  -0.497    0.624    
## F_T_G   5544.8    19725.4   0.281    0.781    
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 1048 on 23 degrees of freedom
## Multiple R-squared:  0.9838, Adjusted R-squared:  0.9789 
## F-statistic: 200.1 on 7 and 23 DF,  p-value: < 2.2e-16


It is clear that all the coefficients related to the 4 interactions are statistically not significant therefore I remove the variable with the greater P-value and I repeat the procedure (this because the three starting vectors are linearly dependent in this kind of model).


model = lm(Viscosity_cP~ 0+FSC+TARA+GUAR+F_T+F_G+T_G, df_complete)
summary(model)
## 
## Call:
## lm(formula = Viscosity_cP ~ 0 + FSC + TARA + GUAR + F_T + F_G + 
##     T_G, data = df_complete)
## 
## Residuals:
##      Min       1Q   Median       3Q      Max 
## -1891.56  -730.02    92.47   622.26  2298.44 
## 
## Coefficients:
##      Estimate Std. Error t value Pr(>|t|)    
## FSC    6276.9      558.2  11.245 4.74e-11 ***
## TARA   9078.7      558.2  16.265 1.84e-14 ***
## GUAR   5061.3      558.2   9.068 3.21e-09 ***
## F_T    2733.3     2471.1   1.106    0.280    
## F_G    2847.5     2471.1   1.152    0.261    
## T_G   -1071.8     2471.1  -0.434    0.668    
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 1027 on 24 degrees of freedom
## Multiple R-squared:  0.9838, Adjusted R-squared:  0.9797 
## F-statistic: 242.7 on 6 and 24 DF,  p-value: < 2.2e-16

Also F_T is removed

model = lm(Viscosity_cP~ 0+FSC+TARA+GUAR+F_G+T_G, df_complete)
summary(model)
## 
## Call:
## lm(formula = Viscosity_cP ~ 0 + FSC + TARA + GUAR + F_G + T_G, 
##     data = df_complete)
## 
## Residuals:
##      Min       1Q   Median       3Q      Max 
## -1992.78  -699.19   -65.49   499.26  2197.22 
## 
## Coefficients:
##      Estimate Std. Error t value Pr(>|t|)    
## FSC    6580.6      488.1  13.481 5.70e-13 ***
## TARA   9382.4      488.1  19.220  < 2e-16 ***
## GUAR   5061.3      560.7   9.027 2.42e-09 ***
## F_G    2391.8     2447.4   0.977    0.338    
## T_G   -1527.4     2447.4  -0.624    0.538    
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 1032 on 25 degrees of freedom
## Multiple R-squared:  0.983,  Adjusted R-squared:  0.9796 
## F-statistic: 288.4 on 5 and 25 DF,  p-value: < 2.2e-16

Then T_G

## 
## Call:
## lm(formula = Viscosity_cP ~ 0 + FSC + TARA + GUAR + F_G, data = df_complete)
## 
## Residuals:
##      Min       1Q   Median       3Q      Max 
## -2177.04  -701.62   -50.49   563.24  2012.96 
## 
## Coefficients:
##      Estimate Std. Error t value Pr(>|t|)    
## FSC    6609.7      480.2   13.77 1.89e-13 ***
## TARA   9237.0      423.9   21.79  < 2e-16 ***
## GUAR   4886.8      480.2   10.18 1.47e-10 ***
## F_G    2610.1     2393.7    1.09    0.286    
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 1020 on 26 degrees of freedom
## Multiple R-squared:  0.9827, Adjusted R-squared:   0.98 
## F-statistic: 369.1 on 4 and 26 DF,  p-value: < 2.2e-16

And eventually F_G .

## 
## Call:
## lm(formula = Viscosity_cP ~ 0 + FSC + TARA + GUAR, data = df_complete)
## 
## Residuals:
##      Min       1Q   Median       3Q      Max 
## -2206.03  -820.70     2.15   706.55  1983.97 
## 
## Coefficients:
##      Estimate Std. Error t value Pr(>|t|)    
## FSC    6870.7      417.7   16.45 1.36e-15 ***
## TARA   9150.0      417.7   21.90  < 2e-16 ***
## GUAR   5147.8      417.7   12.32 1.35e-12 ***
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 1023 on 27 degrees of freedom
## Multiple R-squared:  0.9819, Adjusted R-squared:  0.9799 
## F-statistic: 488.4 on 3 and 27 DF,  p-value: < 2.2e-16


Coefficients and residuals


The coefficients of my model will therefore be

coefficients(model)
##      FSC     TARA     GUAR 
## 6870.677 9149.960 5147.763

And a value of r² of

summary(model)$r.squared
## [1] 0.9819043


I can also draw a scatter plot that relates the response obtained experimentally with the one calculated by the regression model


residui = residuals(model)

df_visc = data.frame('ID' = as.character(df$ID), 'Week' = as.character(df$Week), 'Visc' = df$Viscosity_cP, 'Visc_calc' = df$Viscosity_cP-residui )
bisettrice = data.frame(x= c(4000,10500),y=c(4000,10500))
fig = ggplot(df_visc, aes(x=Visc, y=Visc_calc, color = Week))+ geom_point(aes(label = ID))+
  #geom_text(label=df_visc$id, size=3, hjust=0, vjust=2)+
  geom_line(data=bisettrice, aes(x,y), colour = 'grey')+
  ggtitle('Sperimentali vs calcolati')+
  theme_minimal()
  #theme(plot.title = element_text(hjust = 0.5))

  ggplotly(fig)


Response surface


Starting from the coefficients obtained from the model I can visualize the response surface.

fsc = df$FSC
tara = df$TARA
guar = df$GUAR

par(mar = rep(0.2, 4))

TernaryPlot(alab='tara',blab =  'guar',clab =  'fsc')


Fu = function(tara, guar, fsc) {
        model$coefficients['FSC']*fsc+
        model$coefficients['GUAR']*guar+
        model$coefficients['TARA']*tara
        
}

values = TernaryPointValues(Fu)
ColourTernary(values)

TernaryContour(Fu, resolution = 36L)


It is clear that the tara gum is the thickener that gives greater viscosity to the mixture at the same weight while the guar gum is the one that has a lower thickening power.



Overrun


Regression

As made for the viscosity, a regression is made to find the optimal coefficients according to the model, evaluating their significance (95% confidence limit).

Being a model relative to a ternary mixture I don’t have the value relative to the intercept as for a traditional linear regression.



model = lm(Overrun~ 0+FSC+TARA+GUAR+F_T+F_G+T_G+F_T_G, df_complete)
summary(model)
## 
## Call:
## lm(formula = Overrun ~ 0 + FSC + TARA + GUAR + F_T + F_G + T_G + 
##     F_T_G, data = df_complete)
## 
## Residuals:
##       Min        1Q    Median        3Q       Max 
## -0.120859 -0.028096  0.005774  0.023291  0.098241 
## 
## Coefficients:
##       Estimate Std. Error t value Pr(>|t|)    
## FSC    0.34487    0.02480  13.908 1.10e-12 ***
## TARA   0.31290    0.02480  12.618 8.05e-12 ***
## GUAR   0.54590    0.02480  22.015  < 2e-16 ***
## F_T    0.14700    0.11591   1.268    0.217    
## F_G   -0.07299    0.11591  -0.630    0.535    
## T_G    0.02117    0.11591   0.183    0.857    
## F_T_G -0.86216    0.85023  -1.014    0.321    
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 0.04515 on 23 degrees of freedom
## Multiple R-squared:  0.9907, Adjusted R-squared:  0.9879 
## F-statistic: 351.3 on 7 and 23 DF,  p-value: < 2.2e-16


It is clear that all the coefficients related to the 4 interactions are statistically not significant therefore I remove the variable with the greater P-value and I repeat the procedure (this because the three starting vectors are linearly dependent in this kind of model).


model = lm(Overrun~ 0+FSC+TARA+GUAR+F_T+F_G+T_G, df_complete)
summary(model)
## 
## Call:
## lm(formula = Overrun ~ 0 + FSC + TARA + GUAR + F_T + F_G + T_G, 
##     data = df_complete)
## 
## Residuals:
##       Min        1Q    Median        3Q       Max 
## -0.115387 -0.022624 -0.000817  0.025591  0.103713 
## 
## Coefficients:
##      Estimate Std. Error t value Pr(>|t|)    
## FSC   0.34852    0.02455  14.197 3.57e-13 ***
## TARA  0.31654    0.02455  12.894 2.78e-12 ***
## GUAR  0.54954    0.02455  22.386  < 2e-16 ***
## F_T   0.10596    0.10868   0.975    0.339    
## F_G  -0.11403    0.10868  -1.049    0.305    
## T_G  -0.01987    0.10868  -0.183    0.856    
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 0.04518 on 24 degrees of freedom
## Multiple R-squared:  0.9903, Adjusted R-squared:  0.9879 
## F-statistic: 409.2 on 6 and 24 DF,  p-value: < 2.2e-16

Also F_T is removed

model = lm(Overrun~ 0+FSC+TARA+GUAR+F_G+T_G, df_complete)
summary(model)
## 
## Call:
## lm(formula = Overrun ~ 0 + FSC + TARA + GUAR + F_G + T_G, data = df_complete)
## 
## Residuals:
##       Min        1Q    Median        3Q       Max 
## -0.119311 -0.022005  0.002922  0.025843  0.099789 
## 
## Coefficients:
##      Estimate Std. Error t value Pr(>|t|)    
## FSC   0.36029    0.02135  16.874 3.57e-15 ***
## TARA  0.32832    0.02135  15.376 2.99e-14 ***
## GUAR  0.54954    0.02452  22.408  < 2e-16 ***
## F_G  -0.13169    0.10706  -1.230    0.230    
## T_G  -0.03754    0.10706  -0.351    0.729    
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 0.04514 on 25 degrees of freedom
## Multiple R-squared:  0.9899, Adjusted R-squared:  0.9879 
## F-statistic: 491.8 on 5 and 25 DF,  p-value: < 2.2e-16

Then F_G

## 
## Call:
## lm(formula = Overrun ~ 0 + FSC + TARA + GUAR + T_G, data = df_complete)
## 
## Residuals:
##       Min        1Q    Median        3Q       Max 
## -0.120148 -0.018338 -0.003353  0.028751  0.098952 
## 
## Coefficients:
##      Estimate Std. Error t value Pr(>|t|)    
## FSC   0.34775    0.01895  18.355  < 2e-16 ***
## TARA  0.33082    0.02146  15.413 1.36e-14 ***
## GUAR  0.53449    0.02146  24.902  < 2e-16 ***
## T_G  -0.01872    0.10700  -0.175    0.862    
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 0.04558 on 26 degrees of freedom
## Multiple R-squared:  0.9893, Adjusted R-squared:  0.9877 
## F-statistic: 602.5 on 4 and 26 DF,  p-value: < 2.2e-16

And eventually T_G .

## 
## Call:
## lm(formula = Overrun ~ 0 + FSC + TARA + GUAR, data = df_complete)
## 
## Residuals:
##       Min        1Q    Median        3Q       Max 
## -0.122436 -0.018130 -0.003145  0.030207  0.096664 
## 
## Coefficients:
##      Estimate Std. Error t value Pr(>|t|)    
## FSC   0.34838    0.01827   19.07   <2e-16 ***
## TARA  0.32895    0.01827   18.00   <2e-16 ***
## GUAR  0.53262    0.01827   29.15   <2e-16 ***
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 0.04475 on 27 degrees of freedom
## Multiple R-squared:  0.9893, Adjusted R-squared:  0.9881 
## F-statistic: 833.2 on 3 and 27 DF,  p-value: < 2.2e-16


Coefficients and residuals


The coefficients of my model will therefore be

coefficients(model)
##       FSC      TARA      GUAR 
## 0.3483774 0.3289526 0.5326228

And a value of r² of

summary(model)$r.squared
## [1] 0.9893134


I can also draw a scatter plot that relates the response obtained experimentally with the one calculated by the regression model


residui = residuals(model)

df_overrun = data.frame('ID' = as.character(df$ID), 'Week' = as.character(df$Week), 'Overrun' = df$Overrun, 'Overrun_calc' = df$Overrun-residui )
bisettrice = data.frame(x= c(0.25,0.6),y=c(0.25,0.6))
fig = ggplot(df_overrun, aes(x=Overrun, y=Overrun_calc, color = Week))+ geom_point(aes(label = ID))+
  #geom_text(label=df_visc$id, size=3, hjust=0, vjust=2)+
  geom_line(data=bisettrice, aes(x,y), colour = 'grey')+
  ggtitle('Sperimentali vs calcolati')+
  theme_minimal()
  #theme(plot.title = element_text(hjust = 0.5))

  ggplotly(fig)


Response surface


Starting from the coefficients obtained from the model I can visualize the response surface.

fsc = df$FSC
tara = df$TARA
guar = df$GUAR

par(mar = rep(0.2, 4))

TernaryPlot(alab='tara',blab =  'guar',clab =  'fsc')


Fu = function(tara, guar, fsc) {
        model$coefficients['FSC']*fsc+
        model$coefficients['GUAR']*guar+
        model$coefficients['TARA']*tara
        
}

values = TernaryPointValues(Fu)
ColourTernary(values)

TernaryContour(Fu, resolution = 36L)


As for the overrun, there seems to be an inverse correlation with the viscosity. // This assumption can be verified by correlating the two response variables.


df2 = data.frame(df[c("ID", "Week", "Viscosity_cP", "Overrun")])

fig = ggplot(df2, aes(x=Viscosity_cP, y=Overrun, color = Week))+ geom_point(aes(label = ID))+
  xlim(2500, 10500) + 
  ggtitle('Viscosity vs Overrun')+
  theme_minimal()  
  #theme(plot.title = element_text(hjust = 0.5))

  ggplotly(fig)


---
title: "Thickeners for gelato mixtures"
author: "Arturo Frisina"
subtitle: DOE and linear regression model
output:
  html_document: 
    theme: cerulean
    toc: yes
    code_folding: hide
    code_download: yes
    keep_md: yes
---

```{r Libraries, message=FALSE, warning=FALSE, include=FALSE}
library(readxl)
library(tidyverse)
library(ggtern)
#library(janitor)
library(Ternary)
library(kableExtra)
library(plotly)
library(shiny)

```

<br/>

## Setting up the experimental design

<br/>

We wanted to evaluate the effects of three thickeners of a generic ice cream mix on the **viscosity** of the mix and on the **overrun** of the finished ice cream, two parameters that influences in an important way the characteristics of the finished product.

We examined three thickeners commonly used as food additives:

-   E410 - Locust bean gum or carob seed flour (FSC)
-   E417 - Tara gum (TARA)
-   E412 - Guar gum (GUAR)

We set up a mixture design of the Simplex Lattice type with **k=3** and **m=3**, whose possible combinations led to carrying out 10 experimental conditions. We performed 3 replicates in 3 different weeks, although for this analysis we chose to consider only the last two sets of replicates..

<br/>

<hr/>

```{r echo=TRUE}

df = read.csv("AddensantiDOE.csv", sep = ";")
week = rep(c(1,2,3), each=10 ) %>% factor()
df = add_column(df, Week = week, .after = "ID")


kable(df, row.names = T) %>% kable_styling('striped', fixed_thead = T, full_width = FALSE) %>%
  scroll_box( height = "500px")


```

<br/>

## Postuleted model

<br/>

Once the experiments have been carried out the data can be processed according to a simplified **Scheffè model** (*special cubic*), which allows to take into account the effects given by the possible interactions between the 3 variables FSC, TARA and GUAR.

The model is as follows:

$$
  Y = b_0+b_1x_1+b_2x_2+b_3x_3+b_{12}x_1x_2+b_{13}x_1x_3+b_{23}x_2x_3+b_{123}x_1x_2x_3
$$\

Additional columns related to 2-components interaction and 3-component interaction are then added to the starting dataset.\
<br/>

```{r echo=FALSE, warning=FALSE}

df$F_T = df$FSC*df$TARA
df$T_G = df$TARA*df$GUAR
df$F_G = df$FSC*df$GUAR
df$F_T_G = df$FSC*df$TARA*df$GUAR

df_complete = relocate(df, Viscosity_cP, Overrun, .after = last_col())

kable(df_complete, row.names = T, digits = 4) %>% kable_styling('striped', fixed_thead = T, full_width = FALSE) %>%
  scroll_box( height = "500px")


```

------------------------------------------------------------------------

## Viscosity

<br/>

### Regression

A regression is made to find the optimal coefficients according to the model, evaluating their significance (95% confidence limit).

Being a model relative to a ternary mixture I don't have the value relative to the intercept as for a traditional linear regression.

<hr/>

<br/>

```{r echo=TRUE}

model = lm(Viscosity_cP~ 0+FSC+TARA+GUAR+F_T+F_G+T_G+F_T_G, df_complete)
summary(model)


```

<br/>

It is clear that all the coefficients related to the 4 interactions are statistically not significant therefore I remove the variable with the greater **P-value** and I repeat the procedure (this because the three starting vectors are linearly dependent in this kind of model).

------------------------------------------------------------------------

\tiny

```{r echo=TRUE}

model = lm(Viscosity_cP~ 0+FSC+TARA+GUAR+F_T+F_G+T_G, df_complete)
summary(model)
```

Also `F_T` is removed

```{r echo=TRUE}
model = lm(Viscosity_cP~ 0+FSC+TARA+GUAR+F_G+T_G, df_complete)
summary(model)
```

Then `T_G`

```{r echo=FALSE}
model = lm(Viscosity_cP~ 0+FSC+TARA+GUAR+F_G, df_complete)
summary(model)
```

And eventually `F_G` .\

```{r echo=FALSE}
model = lm(Viscosity_cP ~ 0 + FSC + TARA + GUAR, df_complete)
summary(model)

```

<br/>

### Coefficients and residuals

<br/>

The coefficients of my model will therefore be

```{r echo=TRUE}

coefficients(model)

```

And a value of r² of

```{r echo=TRUE}
summary(model)$r.squared

```

<br/>

I can also draw a scatter plot that relates the response obtained experimentally with the one calculated by the regression model

<br/>

```{r echo=TRUE}
residui = residuals(model)

df_visc = data.frame('ID' = as.character(df$ID), 'Week' = as.character(df$Week), 'Visc' = df$Viscosity_cP, 'Visc_calc' = df$Viscosity_cP-residui )
bisettrice = data.frame(x= c(4000,10500),y=c(4000,10500))

```

<center>

```{r Scatter visc, echo=TRUE, fig.align='center', message=FALSE, warning=FALSE}

fig = ggplot(df_visc, aes(x=Visc, y=Visc_calc, color = Week))+ geom_point(aes(label = ID))+
  #geom_text(label=df_visc$id, size=3, hjust=0, vjust=2)+
  geom_line(data=bisettrice, aes(x,y), colour = 'grey')+
  ggtitle('Sperimentali vs calcolati')+
  theme_minimal()
  #theme(plot.title = element_text(hjust = 0.5))

  ggplotly(fig)


```

</center>

<hr/>

<br/>

### Response surface

<br/>

Starting from the coefficients obtained from the model I can visualize the response surface.

```{r, fig.align='center',echo=TRUE}

fsc = df$FSC
tara = df$TARA
guar = df$GUAR

par(mar = rep(0.2, 4))

TernaryPlot(alab='tara',blab =  'guar',clab =  'fsc')


Fu = function(tara, guar, fsc) {
        model$coefficients['FSC']*fsc+
        model$coefficients['GUAR']*guar+
        model$coefficients['TARA']*tara
        
}

values = TernaryPointValues(Fu)
ColourTernary(values)

TernaryContour(Fu, resolution = 36L)


```

<br/>

It is clear that the tara gum is the thickener that gives greater viscosity to the mixture at the same weight while the guar gum is the one that has a lower thickening  power. 

<hr/>

<br/>

## Overrun

<br/>

### Regression

As made for the viscosity, a regression is made to find the optimal coefficients according to the model, evaluating their significance (95% confidence limit).

Being a model relative to a ternary mixture I don't have the value relative to the intercept as for a traditional linear regression.

<hr/>

<br/>

```{r echo=TRUE}

model = lm(Overrun~ 0+FSC+TARA+GUAR+F_T+F_G+T_G+F_T_G, df_complete)
summary(model)


```

<br/>

It is clear that all the coefficients related to the 4 interactions are statistically not significant therefore I remove the variable with the greater **P-value** and I repeat the procedure (this because the three starting vectors are linearly dependent in this kind of model).

------------------------------------------------------------------------

\tiny

```{r echo=TRUE}

model = lm(Overrun~ 0+FSC+TARA+GUAR+F_T+F_G+T_G, df_complete)
summary(model)
```

Also `F_T` is removed

```{r echo=TRUE}
model = lm(Overrun~ 0+FSC+TARA+GUAR+F_G+T_G, df_complete)
summary(model)
```

Then `F_G`

```{r echo=FALSE}
model = lm(Overrun~ 0+FSC+TARA+GUAR+T_G, df_complete)
summary(model)
```

And eventually `T_G` .\

```{r echo=FALSE}

model = lm(Overrun~ 0+FSC+TARA+GUAR, df_complete)
summary(model)

```

<br/>

### Coefficients and residuals

<br/>

The coefficients of my model will therefore be

```{r echo=TRUE}

coefficients(model)

```

And a value of r² of

```{r echo=TRUE}
summary(model)$r.squared

```

<br/>

I can also draw a scatter plot that relates the response obtained experimentally with the one calculated by the regression model

<br/>

```{r echo=TRUE}
residui = residuals(model)

df_overrun = data.frame('ID' = as.character(df$ID), 'Week' = as.character(df$Week), 'Overrun' = df$Overrun, 'Overrun_calc' = df$Overrun-residui )
bisettrice = data.frame(x= c(0.25,0.6),y=c(0.25,0.6))

```

<center>

```{r Scatter plot, echo=TRUE, fig.align='center', message=FALSE, warning=FALSE}

fig = ggplot(df_overrun, aes(x=Overrun, y=Overrun_calc, color = Week))+ geom_point(aes(label = ID))+
  #geom_text(label=df_visc$id, size=3, hjust=0, vjust=2)+
  geom_line(data=bisettrice, aes(x,y), colour = 'grey')+
  ggtitle('Sperimentali vs calcolati')+
  theme_minimal()
  #theme(plot.title = element_text(hjust = 0.5))

  ggplotly(fig)


```

</center>

<hr/>

<br/>

### Response surface

<br/>

Starting from the coefficients obtained from the model I can visualize the response surface.

```{r, fig.align='center',echo=TRUE}

fsc = df$FSC
tara = df$TARA
guar = df$GUAR

par(mar = rep(0.2, 4))

TernaryPlot(alab='tara',blab =  'guar',clab =  'fsc')


Fu = function(tara, guar, fsc) {
        model$coefficients['FSC']*fsc+
        model$coefficients['GUAR']*guar+
        model$coefficients['TARA']*tara
        
}

values = TernaryPointValues(Fu)
ColourTernary(values)

TernaryContour(Fu, resolution = 36L)


```

<br/>

As for the overrun, there seems to be an inverse correlation with the viscosity. //
This assumption can be verified by correlating the two response variables.

<br/>

<center>

```{r Scatter plot visc_over, echo=TRUE, fig.align='center', message=FALSE, warning=FALSE}

df2 = data.frame(df[c("ID", "Week", "Viscosity_cP", "Overrun")])

fig = ggplot(df2, aes(x=Viscosity_cP, y=Overrun, color = Week))+ geom_point(aes(label = ID))+
  xlim(2500, 10500) + 
  ggtitle('Viscosity vs Overrun')+
  theme_minimal()  
  #theme(plot.title = element_text(hjust = 0.5))

  ggplotly(fig)


```

</center>
<br/>


