Category: Numerical Analysis
Blog Entry © Tuesday, January 7 – Thursday, January 9, 2025, by James Pate Williams, Jr. Solution of a System of Nonlinear Equations Using Damped Newton’s Method for a System of Equations
Blog Entry © Tuesday, January 7, 2025, by James Pate Williams, Jr.
Blog Entry © Wednesday, January 1, 2025, by James Pate Williams, Jr Solution of a 4×4 System of Nonlinear Equations Using a Homegrown Evolutionary Hill-Climber
Live Person-to-Person Tutoring
First United Methodist Church (FUMC) of LaGrange Georgia Historical Attendance Data for the Year of 2006 © James Pate Williams, Jr., BA, BS, Master Software Engineering, PhD and FUMC Friday, December 20, 2024, to Tuesday, December 24, 2024
Blog Entry (c) Wednesday, December 18, 2024, Curve Fitting Using Orthogonal Polynomials by James Pate Williams, Jr.
Blog Entry © Saturday, November 30, 2024, by James Pate Williams, Jr. Partial Solution of the Schrödinger Equation for Hydrogen in Parabolic Coordinates
Blog Entry (c) Thursday, November 21, 2024, by James Pate Williams, Jr. Comparison of Homegrown Fifth Order Runge-Kutta Method Versus a Limited Number of Predictor-Corrector Algorithm
The first table is based on Conte-de Boor Fourth Runge-Kutta formulas that I converted to Fifth Order Runge-Kutta. Initial values: V = 2600 feet per second angle of elevation 30 degrees diameter 16 inches coefficient of form 0.61 density ratio 1.00 are from LCDR Ernest Edward Herrmann’s Exterior ballistics, 1935 My results are given first then LCDR Herrmann’s results:
| x | deg | min | sec | time | v | vx | vy | y |
|---|---|---|---|---|---|---|---|---|
| 0 | 30 | 0 | 0 | 0.00 | 2600 | 2252 | 1300 | 0 |
| 563 | 29 | 50 | 45 | 0.25 | 2578 | 2236 | 1283 | 325 |
| 1122 | 29 | 41 | 24 | 0.50 | 2556 | 2221 | 1266 | 646 |
| 1677 | 29 | 31 | 57 | 0.75 | 2535 | 2206 | 1250 | 962 |
| 2229 | 29 | 22 | 25 | 1.00 | 2515 | 2191 | 1233 | 1275 |
| 2776 | 29 | 12 | 47 | 1.25 | 2494 | 2177 | 1217 | 1583 |
| 3321 | 29 | 3 | 4 | 1.50 | 2474 | 2163 | 1201 | 1887 |
| 3861 | 28 | 53 | 15 | 1.75 | 2455 | 2149 | 1186 | 2188 |
| x | deg | min | sec | time | v | vx | vy | y |
|---|---|---|---|---|---|---|---|---|
| 0 | 30 | 0 | 0 | 0.00 | 2600 | 2252 | 1300 | 0 |
| 561 | 29 | 50 | 7 | 0.25 | 2582 | 2259 | 1285 | 323 |
| 1120 | 29 | 41 | 4 | 0.50 | 2564 | 2227 | 1270 | 642 |
| 1675 | 29 | 32 | 2 | 0.75 | 2546 | 2216 | 1255 | 958 |
| 2228 | 29 | 22 | 5 | 1.00 | 2529 | 2204 | 1241 | 1270 |
It is amazing how accurate Herrmann’s results were based on only a couple iterations using the Mayevski seven zone velocity retardation formulas.