Research Article

Solitary Wave Solutions for a Time-Fraction Generalized Hirota-Satsuma Coupled KdV Equation by a New Analytical Technique

Table 2

Numerical values when , 0.75, 1.0 and , , , for .


0.20−3.004851885−3.009951963−3.010186962−3.011485031−3.013961813−3.013960000−3.013961811
0.25−2.999873282−3.004930481−3.005175951−3.006462592−3.008937820−3.008936014−3.008937819
0.5−2.994919279−2.999927784−3.000183326−3.001457026−3.003927607−3.003925818−3.003927606
0.75−2.989995777−2.994950010−2.995215173−2.996474487−2.998937350−2.998935586−2.998937348
1−2.985108534−2.990003168−2.990277460−2.991521007−2.993973118−2.993971391−2.993973120

0.40−2.998707345−3.001587258−3.003540427−3.004319121−3.007934500−3.007920000−3.007934475
0.25−2.993774914−2.996584581−2.998560913−2.999314737−3.002927784−3.002913367−3.002927763
0.5−2.988873896−2.991611047−2.993607731−2.994336092−2.997942249−2.997927984−2.997942228
0.75−2.984009951−2.986672646−2.988686777−2.989389199−2.992983946−2.992969899−2.992983924
1−2.979188572−2.981775197−2.983803790−2.984479922−2.988058789−2.988045031−2.988058768

0.60−2.994081735−2.994318388−2.997767879−2.997835535−3.001928965−3.001880000−3.001928766
0.25−2.989192682−2.989342884−2.992826759−2.992857834−2.996948389−2.996899772−2.996948197
0.5−2.984339775−2.984405468−2.987918608−2.987913837−2.991996239−2.991948208−2.991996054
0.75−2.979528475−2.979511953−2.983049116−2.983009390−2.987078404−2.987031190−2.987078224
1−2.974764060−2.974667936−2.978223778−2.978150144−2.982200600−2.982154433−2.982200431