Regulation method of easy dyeing for patterning four-component chenille carpet pile

Abstract

The regulation method of easy dyeing for patterning a four-component chenille carpet pile combines raw filaments with different dyeing properties to prepare chenille yarns, and changes the combination modes and ratios of the raw filaments to prepare a four-component chenille carpet pile. The method realizes the heterochromaticity of the four-component pile through the uneven distribution of different dyes on the four-component raw filaments, and regulates the color difference of the four-component filaments after dyeing to form patterns with hazy, moderate and clear color mixing effects. The mixing of different colors dyed on the fibers in the four-component chenille carpet pile is spatial juxtaposition mixing, which forms a non-uniform and constant mixed color. According to the different mixing ratios of the color fibers and the interaction between the fiber hues, a composite color consisting of dominant and secondary hues is produced, thereby presenting a dynamic color.

Claims

1. A regulation method of dyeing for patterning a four-component chenille carpet pile, comprising the following steps: step A: providing four types of raw filaments α, β, γ, δ with equal linear densities and different dyeing properties; mixing the four types of the raw filaments α, β, γ, δ to obtain multiple types of pile filaments corresponding to different combinations of a specified number of the raw filaments α, β, γ, δ, forming a four-component chenille carpet pile filament system; and proceeding to step B; step B: using four preset types of dyes with the different dyeing properties and different base colors that are respectively applicable to the raw filaments α, β, γ, δ to dye the multiple types of pile filaments corresponding to the different combinations of a specified number of the raw filaments α, β, γ, δ, thereby obtaining dyed raw filaments α, β, γ, δ in the multiple types of pile filaments respectively; and proceeding to step C; step C: calculating, based on red, green and blue (RGB) values (R.sub.α, G.sub.α, B.sub.α), (R.sub.β, G.sub.β, B.sub.β), (R.sub.γ, G.sub.γ, B.sub.γ) and (R.sub.δ, G.sub.δ, B.sub.δ) of the dyed raw filaments α, β, γ, δ in the multiple types of pile filaments corresponding to the different combinations of the specified number of the raw filaments α, β, γ, δ, RGB values of the multiple types of pile filaments corresponding to the different combinations of the specified number of the raw filaments α, β, γ, δ, thereby calculating RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of a chenille carpet pile ξ corresponding to the different combinations of the specified number of the raw filaments α, β, γ, δ; and proceeding to step D; and step D: selecting combinations of four base colors with preset hue differences from preset base colors; dyeing, by the combinations of the four base colors, the raw filaments α, β, γ, δ in the multiple types of pile filaments respectively according to step B to obtain multiple types of mixed-color pile filaments with the preset hue differences; and constructing, according to the RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to the different combinations of the specified number of the raw filaments α, β, γ, δ, preset types of chenille carpet piles by tufting the multiple types of mixed-color pile filaments with the preset hue differences.

2. The regulation method according to claim 1, wherein step A comprises: providing the four types of the raw filaments α, β, γ, δ with the equal linear densities and the different dyeing properties, as shown in Table 1; and TABLE-US-00013 TABLE 1 Numbers of raw filaments 4 filaments 6 filaments 8 filaments Combinations α β γ δ α β γ δ α β γ δ 1 1/4 1/4 1/4 1/4 3/6 1/6 1/6 1/6 5/8 1/8 1/8 1/8 2 2/6 2/6 1/6 1/6 4/8 2/8 1/8 1/8 3 2/6 1/6 2/6 1/6 4/8 1/8 2/8 1/8 4 2/6 1/6 1/6 2/6 4/8 1/8 1/8 2/8 5 1/6 3/6 1/6 1/6 3/8 3/8 1/8 1/8 6 1/6 2/6 2/6 1/6 3/8 2/8 2/8 1/8 7 1/6 2/6 1/6 2/6 3/8 2/8 1/8 2/8 8 1/6 1/6 3/6 1/6 3/8 1/8 3/8 1/8 9 1/6 1/6 2/6 2/6 3/8 1/8 2/8 2/8 10 1/6 1/6 1/6 3/6 3/8 1/8 1/8 3/8 11 2/8 4/8 1/8 1/8 12 2/8 3/8 2/8 1/8 13 2/8 3/8 1/8 2/8 14 2/8 2/8 3/8 1/8 15 2/8 2/8 2/8 2/8 16 2/8 2/8 1/8 3/8 17 2/8 1/8 4/8 1/8 18 2/8 1/8 3/8 2/8 19 2/8 1/8 2/8 3/8 20 2/8 1/8 1/8 4/8 21 1/8 5/8 1/8 1/8 22 1/8 4/8 2/8 1/8 23 1/8 4/8 1/8 2/8 24 1/8 3/8 3/8 1/8 25 1/8 3/8 2/8 2/8 26 1/8 3/8 1/8 3/8 27 1/8 2/8 4/8 1/8 28 1/8 2/8 3/8 2/8 29 1/8 2/8 2/8 3/8 30 1/8 2/8 1/8 4/8 31 1/8 1/8 5/8 1/8 32 1/8 1/8 4/8 2/8 33 1/8 1/8 3/8 3/8 34 1/8 1/8 2/8 4/8 35 1/8 1/8 1/8 5/8 mixing the four types of the raw filaments α, β, γ, δ to obtain the pile filaments with the different combinations of the specified number of the raw filaments α, β, γ, δ and forming the four-component chenille carpet pile filament system.

3. The regulation method according to claim 1, wherein when the specified number of the raw filaments α, β, γ, δ is four, step C comprises: based on Table 2, TABLE-US-00014 TABLE 2 RGB values after combination Combinations R.sub.ξ G.sub.ξ B.sub.ξ 1α + 1β + 1γ + 1δ $\frac{1}{4}*R_{\alpha }+\frac{1}{4}*R_{\beta }+\frac{1}{4}*R_{\gamma }+\frac{1}{4}*R_{\delta }$ $\frac{1}{4}*G_{\alpha }+\frac{1}{4}*G_{\beta }+\frac{1}{4}*G_{\gamma }+\frac{1}{4}*G_{\delta }$ $\frac{1}{4}*B_{\alpha }+\frac{1}{4}*B_{\beta }+\frac{1}{4}*B_{\gamma }+\frac{1}{4}*B_{\delta }$ calculating the RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to the different combinations of the four raw filaments α, β, γ, δ.

4. The regulation method according to claim 1, wherein when the specified number of the raw filaments α, β, γ, δ is six, step C comprises: based on Table 3, TABLE-US-00015 TABLE 3 RGB values after combination Combinations R.sub.ξ G.sub.ξ B.sub.ξ 3α + 1β + 1γ + 1δ $\frac{3}{6}*R_{𝔞}+\frac{1}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ $\frac{3}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ $\frac{3}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 2α + 2β + 1γ + 1δ $\frac{2}{6}*R_{\alpha }+\frac{2}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ $\frac{2}{6}*G_{\alpha }+\frac{2}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ $\frac{2}{6}*B_{\alpha }+\frac{2}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 2α + 1β + 2γ + 1δ $\frac{2}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{2}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ $\frac{2}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{2}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ $\frac{2}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{2}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 2α + 1β + 1γ + 2δ $\frac{2}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{2}{6}*R_{\delta }$ $\frac{2}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{2}{6}*G_{\delta }$ $\frac{2}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{2}{6}*B_{\delta }$ 1α + 3β + 1γ + 1δ $\frac{1}{6}*R_{\alpha }+\frac{3}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ $\frac{1}{6}*G_{\alpha }+\frac{3}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ $\frac{1}{6}*B_{\alpha }+\frac{3}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 1α + 2β + 2γ + 1δ $\frac{1}{6}*R_{\alpha }+\frac{2}{6}*R_{\beta }+\frac{2}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ $\frac{1}{6}*G_{\alpha }+\frac{2}{6}*G_{\beta }+\frac{2}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ $\frac{1}{6}*B_{\alpha }+\frac{2}{6}*B_{\beta }+\frac{2}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 1α + 2β + 1γ + 2δ $\frac{1}{6}*R_{\alpha }+\frac{2}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{2}{6}*R_{\delta }$ $\frac{1}{6}*G_{\alpha }+\frac{2}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{2}{6}*G_{\delta }$ $\frac{1}{6}*B_{\alpha }+\frac{2}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{2}{6}*B_{\delta }$ 1α + 1β + 3γ + 1δ $\frac{1}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{3}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ $\frac{1}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{3}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ $\frac{1}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{3}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 1α + 1β + 2γ + 2δ $\frac{1}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{2}{6}*R_{\gamma }+\frac{2}{6}*R_{\delta }$ $\frac{1}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{2}{6}*G_{\gamma }+\frac{2}{6}*G_{\delta }$ $\frac{1}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{2}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 1α + 1β + 1γ + 3δ $\frac{1}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{3}{6}*R_{\delta }$ $\frac{1}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{3}{6}*G_{\delta }$ $\frac{1}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{3}{6}*B_{\delta }$ calculating the RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to different combinations of six raw filaments α, β, γ, δ.

5. The regulation method according to claim 1, wherein when the specified number of the raw filaments α, β, γ, δ is eight, step C comprises: based on Table 4, TABLE-US-00016 TABLE 4 RGB values after combination Combinations R.sub.ξ G.sub.ξ B.sub.ξ 5α + 1β + 1γ + 1δ $\frac{5}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{5}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{5}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 4α + 2β + 1γ + 1δ $\frac{4}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{4}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{4}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 4α + 1β + 2γ + 1δ $\frac{4}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{4}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{4}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 4α + 1β + 1γ + 2δ $\frac{4}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{4}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{4}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 3α + 3β + 1γ + 1δ $\frac{3}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{3}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{3}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 3α + 2β + 2γ + 1δ $\frac{3}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{3}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{3}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 3α + 2β + 1γ + 2δ $\frac{3}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{3}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{3}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 3α + 1β + 3γ + 1δ $\frac{3}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{3}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{3}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 3α + 1β + 2γ + 2δ $\frac{3}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{3}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{3}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 3α + 1β + 1γ + 3δ $\frac{3}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ $\frac{3}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ $\frac{3}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 2α + 4β + 1γ + 1δ $\frac{2}{8}*R_{\alpha }+\frac{4}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{4}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{4}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 2α + 3β + 2γ + 1δ $\frac{2}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 2α + 3β + 1γ + 2δ $\frac{2}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 2α + 2β + 3γ + 1δ $\frac{2}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 2α + 2β + 2γ + 2δ $\frac{2}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 2α + 2β + 1γ + 3δ $\frac{2}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 2α + 1β + 4γ + 1δ $\frac{2}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{4}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{4}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{4}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 2α + 1β + 3γ + 2δ $\frac{2}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 2α + 1β + 2γ + 3δ $\frac{2}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 2α + 1β + 1γ + 4δ $\frac{2}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{4}{8}*R_{\delta }$ $\frac{2}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{4}{8}*G_{\delta }$ $\frac{2}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{4}{8}*B_{\delta }$ 1α + 5β + 1γ + 1δ $\frac{1}{8}*R_{\alpha }+\frac{5}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{5}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{5}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 4β + 2γ + 1δ $\frac{1}{8}*R_{\alpha }+\frac{4}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{4}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{4}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 4β + 1γ + 2δ $\frac{1}{8}*R_{\alpha }+\frac{4}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{4}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{4}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 1α + 3β + 3γ + 1δ $\frac{1}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 3β + 2γ + 2δ $\frac{1}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 1α + 3β + 1γ + 3δ $\frac{1}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{3}{8}*G_6$ $\frac{1}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 1α + 2β + 4γ + 1δ $\frac{1}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{4}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{4}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{4}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 2β + 3γ + 2δ $\frac{1}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 1α + 2β + 2γ + 3δ $\frac{1}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 1α + 2β + 1γ + 4δ $\frac{1}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{4}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{4}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{4}{8}*B_{\delta }$ 1α + 1β + 5γ + 1δ $\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{5}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{5}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{5}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 1β + 4γ + 2δ $\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{4}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{4}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{4}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 1α + 1β + 3γ + 3δ $\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 1α + 1β + 2γ + 4δ $\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{4}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{4}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{4}{8}*B_{\delta }$ 1α + 1β + 1γ + 5δ $\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{5}{8}*R_{\delta }$ $\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{5}{8}*G_{\delta }$ $\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{5}{8}*B_{\delta }$ calculating the RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to different combinations of eight raw filaments α, β, γ, δ.

6. The regulation method according to claim 1, wherein step D comprises: selecting combinations of four base colors with a hue difference of less than 60° from the preset base colors; dyeing, by the combinations of the four base colors, the raw filaments α, β, γ, δ in the multiple types of pile filaments respectively according to step B to obtain multiple types of mixed-color pile filaments with the hue difference of less than 60°; and constructing, based on the RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to the different combinations of the specified number of the raw filaments α, β, γ, δ, a chenille carpet pile with a hazy color mixing effect by tufting the multiple types of mixed-color pile filaments with the hue difference of less than 60°.

7. The regulation method according to claim 1, wherein step D comprises: selecting combinations of four base colors with a hue difference of greater than 60° and less than 120° from the preset base colors; dyeing, by the combinations of the four base colors, the raw filaments α, β, γ, δ in the multiple types of pile filaments respectively according to step B to obtain multiple types of mixed-color pile filaments with the hue difference of greater than 60° and less than 120°; and constructing, based on the RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to the different combinations of the specified number of the raw filaments α, β, γ, δ, a chenille carpet pile with a moderate color mixing effect by tufting the multiple types of mixed-color pile filaments with the hue difference of greater than 60° and less than 120°.

8. The regulation method according to claim 1, wherein step D comprises: selecting combinations of four base colors with a hue difference of greater than 120° and less than 180° from the preset base colors, and selecting combinations of three base colors with the hue difference of greater than 120° and less than 180° from the preset base colors to cooperate with white or black to form combinations of four base colors; dyeing, by the combinations of the four base colors, the raw filaments α, β, γ, δ in the multiple types of pile filaments respectively according to step B to obtain multiple types of mixed-color pile filaments with the hue difference of greater than 120° and less than 180° from the preset base colors; and constructing, based on the RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to the different combinations of the specified number of the raw filaments α, β, γ, δ, a chenille carpet pile with a clear color mixing effect by tufting the multiple types of mixed-color pile filaments with the hue difference of greater than 120° and less than 180° from the preset base colors.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0028] FIG. 1 is a regulation method of easy dyeing for patterning a four-component chenille carpet pile according to the present disclosure.

[0029] FIG. 2 is a schematic diagram of 24 base colors.

[0030] FIG. 3 shows the practical application of the pattern construction of the chenille carpet pile with a gradient change in the hazy color mixing effect.

[0031] FIG. 4 shows the practical application of the pattern construction of the chenille carpet pile with a gradient change in the moderate color mixing effect.

[0032] FIG. 5 shows the practical application of the pattern construction of the chenille carpet pile with a gradient change in the clear color mixing effect.

DETAILED DESCRIPTION OF THE EMBODIMENTS

[0033] The specific implementation of the present disclosure will be further described in detail below with reference to the drawings.

[0034] The present disclosure proposes a regulation method of easy dyeing for patterning a four-component chenille carpet pile. In a practical application, as shown in FIG. 1, the method specifically includes Steps A to D.

[0035] Step A: Provide four types of raw filaments α, β, γ, δ with equal linear densities and different dyeing properties, for example, polyester filaments, cationically dyeable polyester filaments, polyamide filaments, cationically modified viscose filaments, viscose filaments, acrylic filaments and cationically dyeable acrylic filaments, as shown in Table 1:

TABLE-US-00005 TABLE 1 Numbers of raw filaments 4 filaments 6 filaments 8 filaments Combinations α β γ δ α β γ δ α β γ δ 1 1/4 1/4 1/4 1/4 3/6 1/6 1/6 1/6 5/8 1/8 1/8 1/8 2 2/6 2/6 1/6 1/6 4/8 2/8 1/8 1/8 3 2/6 1/6 2/6 1/6 4/8 1/8 2/8 1/8 4 2/6 1/6 1/6 2/6 4/8 1/8 1/8 2/8 5 1/6 3/6 1/6 1/6 3/8 3/8 1/8 1/8 6 1/6 2/6 2/6 1/6 3/8 2/8 2/8 1/8 7 1/6 2/6 1/6 2/6 3/8 2/8 1/8 2/8 8 1/6 1/6 3/6 1/6 3/8 1/8 3/8 1/8 9 1/6 1/6 2/6 2/6 3/8 1/8 2/8 2/8 10 1/6 1/6 1/6 3/6 3/8 1/8 1/8 3/8 11 2/8 4/8 1/8 1/8 12 2/8 3/8 2/8 1/8 13 2/8 3/8 1/8 2/8 14 2/8 2/8 3/8 1/8 15 2/8 2/8 2/8 2/8 16 2/8 2/8 1/8 3/8 17 2/8 1/8 4/8 1/8 18 2/8 1/8 3/8 2/8 19 2/8 1/8 2/8 3/8 20 2/8 1/8 1/8 4/8 21 1/8 5/8 1/8 1/8 22 1/8 4/8 2/8 1/8 23 1/8 4/8 1/8 2/8 24 1/8 3/8 3/8 1/8 25 1/8 3/8 2/8 2/8 26 1/8 3/8 1/8 3/8 27 1/8 2/8 4/8 1/8 28 1/8 2/8 3/8 2/8 29 1/8 2/8 2/8 3/8 30 1/8 2/8 1/8 4/8 31 1/8 1/8 5/8 1/8 32 1/8 1/8 4/8 2/8 33 1/8 1/8 3/8 3/8 34 1/8 1/8 2/8 4/8 35 1/8 1/8 1/8 5/8

[0036] mix the four types of raw filaments α, β, γ, δ through gradient matching to obtain pile filaments with different combinations of specified numbers of raw filaments α, β, γ, δ, which form a four-component chenille carpet pile filament system; and proceed to Step B.

[0037] Step B. Select four base colors from 26 base colors including A.sub.1, A.sub.2, A.sub.3, . . . , A.sub.22, A.sub.23, A.sub.24, white (W) and black (K), where red, green and blue (RGB) values of A.sub.1, A.sub.2, A.sub.3, . . . , A.sub.22, A.sub.23, A.sub.24 (FIG. 2) are shown in Table 8:

TABLE-US-00006 TABLE 8 A1 A2 A3 A4 (255, 0, 0) (255, 64, 0) (255, 128, 0) (255, 191, 0) A5 A6 A7 A8 (255, 255, 0) (191, 255, 0) (128, 255, 0) (64, 255, 0) A9 A10 A11 A12 (0, 255, 0) (0, 255, 64) (0, 255, 128) (0, 255, 191) A13 A14 A15 A16 (0, 255, 255) (0, 191, 255) (0, 128, 255) (0, 64, 255) A17 A18 A19 A20 (0, 0, 255) (64, 0, 255) (128, 0, 255) (191, 0, 255) A21 A22 A23 A24 (255, 0, 255) (255, 0, 191) (255, 0, 128) (255, 0, 64)

[0038] dye the pile filaments, by four types of dyes that are respectively applicable to the raw filaments α, β, γ, δ with different dyeing properties and have different base colors, the multiple types of pile filaments with different combinations of specified numbers of raw filaments α, β, γ, δ, that is, dye the raw filaments α, β, γ, δ in the multiple types of pile filaments respectively; and proceed to Step C. By selecting and combining four base colors from these base colors, C.sub.26.sup.4=14950 quaternary dyeing modes are achieved.

[0039] Step C: Calculate, based on RGB values (R.sub.α, G.sub.α, B.sub.α), (R.sub.β, G.sub.β, B.sub.β), (R.sub.γ, G.sub.γ, B.sub.γ) and (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the dyed raw filaments α, β, γ, δ in the multiple types of pile filaments with different combinations of specified numbers of raw filaments α, β, γ, δ, RGB values of the multiple types of pile filaments with different combinations of specified numbers of raw filaments α, β, γ, δ, that is, calculate RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of a chenille carpet pile ξ corresponding to different combinations of specified numbers of raw filaments α, β, γ, δ; and proceed to step D.

[0040] In a specific practical application of Step C, for example, the RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to different combinations of 4, 6 and 8 raw filaments α, β, γ, δ are calculated, as shown in Table 2.

TABLE-US-00007 TABLE 2 RGB values after combination Combinations R.sub.ξ G.sub.ξ B.sub.ξ 1α + 1β + 1γ + 1δ [00139]$\frac{1}{4}*R_{\alpha }+\frac{1}{4}*R_{\beta }+\frac{1}{4}*R_{\gamma }+\frac{1}{4}*R_{\delta }$ [00140]$\frac{1}{4}*G_{\alpha }+\frac{1}{4}*G_{\beta }+\frac{1}{4}*G_{\gamma }+\frac{1}{4}*G_{\delta }$ [00141]$\frac{1}{4}*B_{\alpha }+\frac{1}{4}*B_{\beta }+\frac{1}{4}*B_{\gamma }+\frac{1}{4}*B_{\delta }$

[0041] RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to different combinations of 4 raw filaments α, β, γ, δ are calculated.

[0042] A design of the chenille carpet pile ξ corresponding to 6 raw filaments is shown in Table 3.

TABLE-US-00008 TABLE 3 RGB values after combination Combinations R.sub.ξ G.sub.ξ B.sub.ξ 3α + 1β + 1γ + 1δ [00142]$\frac{3}{6}*R_{𝔞}+\frac{1}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ [00143]$\frac{3}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ [00144]$\frac{3}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 2α + 2β + 1γ + 1δ [00145]$\frac{2}{6}*R_{𝔞}+\frac{2}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ [00146]$\frac{2}{6}*G_{\alpha }+\frac{2}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ [00147]$\frac{2}{6}*B_{\alpha }+\frac{2}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 2α + 1β + 2γ + 1δ [00148]$\frac{2}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{2}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ [00149]$\frac{2}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{2}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ [00150]$\frac{2}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{2}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 2α + 1β + 1γ + 2δ [00151]$\frac{2}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{2}{6}*R_{\delta }$ [00152]$\frac{2}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{2}{6}*G_{\delta }$ [00153]$\frac{2}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{2}{6}*B_{\delta }$ 1α + 3β + 1γ + 1δ [00154]$\frac{1}{6}*R_{\alpha }+\frac{3}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ [00155]$\frac{1}{6}*G_{\alpha }+\frac{3}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ [00156]$\frac{1}{6}*B_{\alpha }+\frac{3}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 1α + 2β + 2γ + 1δ [00157]$\frac{1}{6}*R_{\alpha }+\frac{2}{6}*R_{\beta }+\frac{2}{6}*R_{\gamma }+\frac{1}{6}*$ [00158]$\frac{1}{6}*G_{\alpha }+\frac{2}{6}*G_{\beta }+\frac{2}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ [00159]$\frac{1}{6}*B_{\alpha }+\frac{2}{6}*B_{\beta }+\frac{2}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 1α + 2β + 1γ + 2δ [00160]$\frac{1}{6}*R_{\alpha }+\frac{2}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{2}{6}*R_{\delta }$ [00161]$\frac{1}{6}*G_{\alpha }+\frac{2}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{2}{6}*G_{\delta }$ [00162]$\frac{1}{6}*B_{\alpha }+\frac{2}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{2}{6}*B_{\delta }$ 1α + 1β + 3γ + 1δ [00163]$\frac{1}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{3}{6}*R_{\gamma }+\frac{1}{6}*R_{\delta }$ [00164]$\frac{1}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{3}{6}*G_{\gamma }+\frac{1}{6}*G_{\delta }$ [00165]$\frac{1}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{3}{6}*B_{\gamma }+\frac{1}{6}*B_{\delta }$ 1α + 1β + 2γ + 2δ [00166]$\frac{1}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{2}{6}*R_{\gamma }+\frac{2}{6}*R_{\delta }$ [00167]$\frac{1}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{2}{6}*G_{\gamma }+\frac{2}{6}*G_{\delta }$ [00168]$\frac{1}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{2}{6}*B_{\gamma }+\frac{2}{6}*B_{\delta }$ 1α + 1β + 1γ + 3δ [00169]$\frac{1}{6}*R_{\alpha }+\frac{1}{6}*R_{\beta }+\frac{1}{6}*R_{\gamma }+\frac{3}{6}*R_{\delta }$ [00170]$\frac{1}{6}*G_{\alpha }+\frac{1}{6}*G_{\beta }+\frac{1}{6}*G_{\gamma }+\frac{3}{6}*G_{\delta }$ [00171]$\frac{1}{6}*B_{\alpha }+\frac{1}{6}*B_{\beta }+\frac{1}{6}*B_{\gamma }+\frac{3}{6}*B_{\delta }$

[0043] RGB values (R.sub.ξ, G.sub.ξ, B.sub.ξ) of the chenille carpet pile ξ corresponding to different combinations of 6 raw filaments α, β, γ, δ are calculated.

[0044] A design of the chenille carpet pile ξ corresponding to 8 raw filaments is shown in Table 4.

TABLE-US-00009 TABLE 4 RGB values after combination Combinations R.sub.ξ G.sub.ξ B.sub.ξ 5α + 1β + 1γ + 1δ [00172]$\frac{5}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00173]$\frac{5}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00174]$\frac{5}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 4α + 2β + 1γ + 1δ [00175]$\frac{4}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00176]$\frac{4}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00177]$\frac{4}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 4α + 1β + 2γ + 1δ [00178]$\frac{4}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00179]$\frac{4}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00180]$\frac{4}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 4α + 1β + 1γ + 2δ [00181]$\frac{4}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00182]$\frac{4}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00183]$\frac{4}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 3α + 3β + 1γ + 1δ [00184]$\frac{3}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00185]$\frac{3}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00186]$\frac{3}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 3α + 2β + 2γ + 1δ [00187]$\frac{3}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00188]$\frac{3}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00189]$\frac{3}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 3α + 2β + 1γ + 2δ [00190]$\frac{3}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00191]$\frac{3}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00192]$\frac{3}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 3α + 1β + 3γ + 1δ [00193]$\frac{3}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00194]$\frac{3}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00195]$\frac{3}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 3α + 1β + 2γ + 2δ [00196]$\frac{3}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00197]$\frac{3}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00198]$\frac{3}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 3α + 1β + 1γ + 3δ [00199]$\frac{3}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ [00200]$\frac{3}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ [00201]$\frac{3}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 2α + 4β + 1γ + 1δ [00202]$\frac{2}{8}*R_{\alpha }+\frac{4}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00203]$\frac{2}{8}*G_{\alpha }+\frac{4}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00204]$\frac{2}{8}*B_{\alpha }+\frac{4}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 2α + 3β + 2γ + 1δ [00205]$\frac{2}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00206]$\frac{2}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00207]$\frac{2}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 2α + 3β + 1γ + 2δ [00208]$\frac{2}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00209]$\frac{2}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00210]$\frac{2}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 2α + 2β + 3γ + 1δ [00211]$\frac{2}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00212]$\frac{2}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00213]$\frac{2}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 2α + 2β + 2γ + 2δ [00214]$\frac{2}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00215]$\frac{2}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00216]$\frac{2}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 2α + 2β + 1γ + 3δ [00217]$\frac{2}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ [00218]$\frac{2}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ [00219]$\frac{2}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 2α + 1β + 4γ + 1δ [00220]$\frac{2}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{4}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00221]$\frac{2}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{4}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00222]$\frac{2}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{4}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 2α + 1β + 3γ + 2δ [00223]$\frac{2}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00224]$\frac{2}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00225]$\frac{2}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 2α + 1β + 2γ + 3δ [00226]$\frac{2}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ [00227]$\frac{2}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ [00228]$\frac{2}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 2α + 1β + 1γ + 4δ [00229]$\frac{2}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{4}{8}*R_{\delta }$ [00230]$\frac{2}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{4}{8}*G_{\delta }$ [00231]$\frac{2}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{4}{8}*B_{\delta }$ 1α + 5β + 1γ + 1δ [00232]$\frac{1}{8}*R_{\alpha }+\frac{5}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00233]$\frac{1}{8}*G_{\alpha }+\frac{5}{8}*G_{\beta }+\frac{1}{8}*G_Y+\frac{1}{8}*G_{\delta }$ [00234]$\frac{1}{8}*B_{\alpha }+\frac{5}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 4β + 2γ + 1δ [00235]$\frac{1}{8}*R_{\alpha }+\frac{4}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00236]$\frac{1}{8}*G_{\alpha }+\frac{4}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00237]$\frac{1}{8}*B_{\alpha }+\frac{4}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 4β + 1γ + 2δ [00238]$\frac{1}{8}*R_{\alpha }+\frac{4}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00239]$\frac{1}{8}*G_{\alpha }+\frac{4}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00240]$\frac{1}{8}*B_{\alpha }+\frac{4}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 1α + 3β + 3γ + 1δ [00241]$\frac{1}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00242]$\frac{1}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00243]$\frac{1}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 3β + 2γ + 2δ [00244]$\frac{1}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00245]$\frac{1}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00246]$\frac{1}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 1α + 3β + 1γ + 3δ [00247]$\frac{1}{8}*R_{\alpha }+\frac{3}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ [00248]$\frac{1}{8}*G_{\alpha }+\frac{3}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ [00249]$\frac{1}{8}*B_{\alpha }+\frac{3}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 1α + 2β + 4γ + 1δ [00250]$\frac{1}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{4}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00251]$\frac{1}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{4}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00252]$\frac{1}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{4}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 2β + 3γ + 2δ [00253]$\frac{1}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00254]$\frac{1}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00255]$\frac{1}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 1α + 2β + 2γ + 3δ [00256]$\frac{1}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ [00257]$\frac{1}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ [00258]$\frac{1}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 1α + 2β + 1γ + 4δ [00259]$\frac{1}{8}*R_{\alpha }+\frac{2}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{4}{8}*R_{\delta }$ [00260]$\frac{1}{8}*G_{\alpha }+\frac{2}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{4}{8}*G_{\delta }$ [00261]$\frac{1}{8}*B_{\alpha }+\frac{2}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{4}{8}*B_{\delta }$ 1α + 1β + 5γ + 1δ [00262]$\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{5}{8}*R_{\gamma }+\frac{1}{8}*R_{\delta }$ [00263]$\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{5}{8}*G_{\gamma }+\frac{1}{8}*G_{\delta }$ [00264]$\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{5}{8}*B_{\gamma }+\frac{1}{8}*B_{\delta }$ 1α + 1β + 4γ + 2δ [00265]$\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{4}{8}*R_{\gamma }+\frac{2}{8}*R_{\delta }$ [00266]$\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{4}{8}*G_{\gamma }+\frac{2}{8}*G_{\delta }$ [00267]$\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{4}{8}*B_{\gamma }+\frac{2}{8}*B_{\delta }$ 1α + 1β + 3γ + 3δ [00268]$\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{3}{8}*R_{\gamma }+\frac{3}{8}*R_{\delta }$ [00269]$\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{3}{8}*G_{\gamma }+\frac{3}{8}*G_{\delta }$ [00270]$\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{3}{8}*B_{\gamma }+\frac{3}{8}*B_{\delta }$ 1α + 1β + 2γ + 4δ [00271]$\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{2}{8}*R_{\gamma }+\frac{4}{8}*R_{\delta }$ [00272]$\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{2}{8}*G_{\gamma }+\frac{4}{8}*G_{\delta }$ [00273]$\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{2}{8}*B_{\gamma }+\frac{4}{8}*B_{\delta }$ 1α + 1β + 1γ + 5δ [00274]$\frac{1}{8}*R_{\alpha }+\frac{1}{8}*R_{\beta }+\frac{1}{8}*R_{\gamma }+\frac{5}{8}*R_{\delta }$ [00275]$\frac{1}{8}*G_{\alpha }+\frac{1}{8}*G_{\beta }+\frac{1}{8}*G_{\gamma }+\frac{5}{8}*G_{\delta }$ [00276]$\frac{1}{8}*B_{\alpha }+\frac{1}{8}*B_{\beta }+\frac{1}{8}*B_{\gamma }+\frac{5}{8}*B_{\delta }$