|
| 1 | +{ |
| 2 | + "cells": [ |
| 3 | + { |
| 4 | + "cell_type": "markdown", |
| 5 | + "id": "72c44810-5086-4a40-8d8a-f825b064f14d", |
| 6 | + "metadata": {}, |
| 7 | + "source": [ |
| 8 | + "# Proof of the R-Formula\n", |
| 9 | + "\n", |
| 10 | + "The main goal is to find a unifying expression for\n", |
| 11 | + "\n", |
| 12 | + "$$\n", |
| 13 | + "a\\sin(x) \\pm b\\cos(x)\n", |
| 14 | + "$$\n", |
| 15 | + "\n", |
| 16 | + "And\n", |
| 17 | + "\n", |
| 18 | + "$$\n", |
| 19 | + "a\\cos(x) \\pm b\\sin(x)\n", |
| 20 | + "$$\n", |
| 21 | + "\n", |
| 22 | + "where\n", |
| 23 | + "$$\n", |
| 24 | + "a > 0 \\quad \\text{and} \\quad b > 0\n", |
| 25 | + "$$" |
| 26 | + ] |
| 27 | + }, |
| 28 | + { |
| 29 | + "cell_type": "markdown", |
| 30 | + "id": "83da1681-d587-498d-9b07-38bac736c4b4", |
| 31 | + "metadata": {}, |
| 32 | + "source": [ |
| 33 | + "# **Cosine First**: $\\mathbf{a\\cos(x) \\pm b\\sin(x)}$\n", |
| 34 | + "\n", |
| 35 | + "\n", |
| 36 | + "## Finding Patterns in Identities\n", |
| 37 | + "\n", |
| 38 | + "Looking through the different trigonometric identities, we can find by that in the double-angle formula\n", |
| 39 | + "\n", |
| 40 | + "$$\n", |
| 41 | + "\\cos(A \\mp B) = \n", |
| 42 | + "\\cos(A)\\cos(B) \\pm \\sin(A)\\sin(B)\n", |
| 43 | + "$$ \n", |
| 44 | + "\n", |
| 45 | + "Its expanded form of \n", |
| 46 | + "\n", |
| 47 | + "$$\n", |
| 48 | + "\\textcolor{lightgray}{\\cos(A \\mp B)} \n", |
| 49 | + "\\textcolor{lightgray}{=} \n", |
| 50 | + "\\textcolor{green}{\\cos(A)}\n", |
| 51 | + "\\cos(B) \n", |
| 52 | + "\\pm \n", |
| 53 | + "\\textcolor{blue}{\\sin(A)}\n", |
| 54 | + "\\sin(B)\n", |
| 55 | + "$$ \n", |
| 56 | + "\n", |
| 57 | + "looks quite similar to:\n", |
| 58 | + "\n", |
| 59 | + "$$\n", |
| 60 | + "\\boxed{\n", |
| 61 | + " \\textcolor{green}{a}\\cos(x) \\pm \\textcolor{blue}{b}\\sin(x)\n", |
| 62 | + "}\n", |
| 63 | + "$$\n", |
| 64 | + "\n", |
| 65 | + "And has the unifying double-angle form of \n", |
| 66 | + "\n", |
| 67 | + "$$\n", |
| 68 | + "\\cos(A \\mp B) = \n", |
| 69 | + "\\textcolor{green}{\\cos(A)} \n", |
| 70 | + "\\textcolor{lightgray}{\\cos(B)} \n", |
| 71 | + "\\textcolor{lightgray}{\\pm}\n", |
| 72 | + "\\textcolor{blue}{\\sin(A)}\n", |
| 73 | + "\\textcolor{lightgray}{\\sin(B)}\n", |
| 74 | + "$$ \n", |
| 75 | + "\n", |
| 76 | + "## Matching Variables\n", |
| 77 | + "\n", |
| 78 | + "To match with $cos(x)$, we can let either let $A = x$ or $B = x$\n", |
| 79 | + "\n", |
| 80 | + "- I choose to let $B = x$\n", |
| 81 | + "\n", |
| 82 | + "$$\n", |
| 83 | + "\\cos(A \\mp x) = \\cos(A)\\cos(x) \\pm \\sin(A)\\sin(x)\n", |
| 84 | + "$$ \n", |
| 85 | + "\n", |
| 86 | + "It may seem that we can match $a$ with $\\cos(A)$ and $b$ with $\\sin(A)$\n", |
| 87 | + "\n", |
| 88 | + "$$\n", |
| 89 | + "\\textcolor{green}{a} \n", |
| 90 | + "\\textcolor{lightgray}{\\cos(x)} \n", |
| 91 | + "\\textcolor{lightgray}{\\pm} \n", |
| 92 | + "\\textcolor{blue}{b} \n", |
| 93 | + "\\textcolor{lightgray}{\\sin(x)} \n", |
| 94 | + "\\textcolor{lightgray}{=} \n", |
| 95 | + "\\textcolor{green}{\\cos(A)} \n", |
| 96 | + "\\textcolor{lightgray}{\\cos(x)} \n", |
| 97 | + "\\textcolor{lightgray}{\\pm} \n", |
| 98 | + "\\textcolor{blue}{\\sin(A)} \n", |
| 99 | + "\\textcolor{lightgray}{\\sin(x)}\n", |
| 100 | + "$$\n", |
| 101 | + "\n", |
| 102 | + "But actually, their ranges do not match.\n", |
| 103 | + "- $sin(A)$ and $cos(A)$ has the range of $[-1, 1]$\n", |
| 104 | + "- While both `a` and `b` has the range of $(0, \\infty)$\n", |
| 105 | + "\n", |
| 106 | + "Therefore, we need a coefficient on the double-angle formula to make the expressions matchable. \n", |
| 107 | + "- We can either have the coefficients individually\n", |
| 108 | + "\n", |
| 109 | + "$$\n", |
| 110 | + "\\textcolor{gray}{p} \n", |
| 111 | + "\\textcolor{lightgray}{\\cos(A)\\cos(x)} \n", |
| 112 | + "\\textcolor{lightgray}{\\pm} \n", |
| 113 | + "\\textcolor{gray}{q} \n", |
| 114 | + "\\textcolor{lightgray}{\\sin(A)\\sin(x)}\n", |
| 115 | + "$$\n", |
| 116 | + "\n", |
| 117 | + "- Or as we are finding unification, we can have some coefficient $R$ on the unified double-angle form, to distribute across the 2 terms\n", |
| 118 | + "\n", |
| 119 | + "$$\n", |
| 120 | + "R\\cos(A \\mp x) = R\\cos(A)\\cos(x) \\pm R\\sin(A)\\sin(x)\n", |
| 121 | + "$$ \n", |
| 122 | + "\n", |
| 123 | + "Now it can have the nice comparison of \n", |
| 124 | + "\n", |
| 125 | + "$$\n", |
| 126 | + "\\textcolor{green}{a}\n", |
| 127 | + "\\textcolor{lightgray}{\\cos(x)}\n", |
| 128 | + "\\textcolor{lightgray}{\\pm}\n", |
| 129 | + "\\textcolor{blue}{b}\n", |
| 130 | + "\\textcolor{lightgray}{\\sin(x)} \n", |
| 131 | + "\\textcolor{lightgray}{=} \n", |
| 132 | + "\\textcolor{green}{R\\cos(A)} \n", |
| 133 | + "\\textcolor{lightgray}{\\cos(x)} \n", |
| 134 | + "\\textcolor{lightgray}{\\pm} \n", |
| 135 | + "\\textcolor{blue}{R\\sin(A)} \n", |
| 136 | + "\\textcolor{lightgray}{\\sin(x)}\n", |
| 137 | + "$$\n", |
| 138 | + "\n", |
| 139 | + "Therefore, we get 2 equations we can work with:\n", |
| 140 | + "\n", |
| 141 | + "$$\n", |
| 142 | + "\\begin{align}\n", |
| 143 | + " a &= R\\cos(A) \\\\\n", |
| 144 | + " b &= R\\sin(A)\n", |
| 145 | + "\\end{align}\n", |
| 146 | + "$$" |
| 147 | + ] |
| 148 | + }, |
| 149 | + { |
| 150 | + "cell_type": "markdown", |
| 151 | + "id": "85684cec-5f4a-4b73-b9a7-9e129e521f4c", |
| 152 | + "metadata": {}, |
| 153 | + "source": [ |
| 154 | + "# Solving for **A** and **R**\n", |
| 155 | + "\n", |
| 156 | + "We want to solve for $A$ and $R$ such that we can complete the unifying formula.\n", |
| 157 | + "\n", |
| 158 | + "\n", |
| 159 | + "## Solving for **A**\n", |
| 160 | + "\n", |
| 161 | + "From the 2 equations, we can find $A$ by combining $\\sin$ and $\\cos$ into $\\tan$:\n", |
| 162 | + "\n", |
| 163 | + "$$\n", |
| 164 | + "\\frac{b}{a} = \\frac{\\cancel{R}\\sin(A)}{\\cancel{R}\\cos(A)} = \\tan(A).\n", |
| 165 | + "$$\n", |
| 166 | + "\n", |
| 167 | + "And then by taking the inverse:\n", |
| 168 | + "\n", |
| 169 | + "$$\n", |
| 170 | + "\\boxed{\n", |
| 171 | + " A = \\arctan\\left(\\frac{b}{a}\\right)\n", |
| 172 | + "}\n", |
| 173 | + "$$\n", |
| 174 | + "\n", |
| 175 | + "- For $\\arctan$, it actually has an infinite domain, so no restrictions here\n", |
| 176 | + "- It is not like $\\arcsin$ or $\\arccos$, where there is an inclusive domain\n", |
| 177 | + "- Or $\\text{arcsec}$ and $\\text{arccsc}$, where there is an exclusive domain\n", |
| 178 | + "- Also notice we could have used $\\cot$ as well in the first place, and then use $\\text{arccot}$\n", |
| 179 | + "\n", |
| 180 | + "$$\n", |
| 181 | + "\\textcolor{lightgray}{\n", |
| 182 | + " \\boxed{\n", |
| 183 | + " A = \\text{arccot} \\left(\\frac{a}{b}\\right)\n", |
| 184 | + " }\n", |
| 185 | + "}\n", |
| 186 | + "$$\n", |
| 187 | + "\n", |
| 188 | + "- But this is a matter of preference\n", |
| 189 | + "\n", |
| 190 | + "Now we have $A$, let's find $R$:\n", |
| 191 | + "\n", |
| 192 | + "## Solving for **R**\n", |
| 193 | + "\n", |
| 194 | + "Going back to the equations:\n", |
| 195 | + "\n", |
| 196 | + "$$\n", |
| 197 | + "a = R\\cos(A), \\quad b = R\\sin(A)\n", |
| 198 | + "$$\n", |
| 199 | + "\n", |
| 200 | + "We can notice that $\\sin(A)$ and $\\cos(A)$ both exist, so we can prepare it to use the Pythagorean identity:\n", |
| 201 | + "\n", |
| 202 | + "$$\n", |
| 203 | + "a^2 = R^2\\cos^2(A), \n", |
| 204 | + "\\quad \n", |
| 205 | + "b^2 = R^2\\sin^2(A)\n", |
| 206 | + "$$\n", |
| 207 | + "\n", |
| 208 | + "> **Take note here**: Because we have squared the equation, we have introduced another extraneous solution into an otherwise single-solution variable\n", |
| 209 | + "\n", |
| 210 | + "\n", |
| 211 | + "Add these together:\n", |
| 212 | + "\n", |
| 213 | + "$$\n", |
| 214 | + "a^2 + b^2 = R^2\\cos^2(A) + R^2\\sin^2(A)\n", |
| 215 | + "$$\n", |
| 216 | + "\n", |
| 217 | + "Factor out $R^2$\n", |
| 218 | + "\n", |
| 219 | + "$$\n", |
| 220 | + "a^2 + b^2 = R^2 \\biggr[ \\cos^2(A) + \\sin^2(A) \\biggr]\n", |
| 221 | + "$$\n", |
| 222 | + "\n", |
| 223 | + "Using the Pythagorean identity $\\cos^2(A) + \\sin^2(A) = 1$:\n", |
| 224 | + "\n", |
| 225 | + "$$\n", |
| 226 | + "a^2 + b^2 = R^2\n", |
| 227 | + "$$\n", |
| 228 | + "\n", |
| 229 | + "Take the square root:\n", |
| 230 | + "\n", |
| 231 | + "$$\n", |
| 232 | + "R = \\pm\\sqrt{a^2 + b^2}\n", |
| 233 | + "$$\n", |
| 234 | + "\n", |
| 235 | + "Thus, right now we have:\n", |
| 236 | + "\n", |
| 237 | + "$$\n", |
| 238 | + "a\\sin(x) \\pm b\\cos(x) = \n", |
| 239 | + "R\\cos(A \\mp x)\n", |
| 240 | + "$$\n", |
| 241 | + "\n", |
| 242 | + "where:\n", |
| 243 | + "\n", |
| 244 | + "$$\n", |
| 245 | + "\\boxed{\n", |
| 246 | + " A = \\arctan\\left(\\frac{b}{a}\\right)\n", |
| 247 | + "}\n", |
| 248 | + "\\quad \\quad \n", |
| 249 | + "R = \\pm\\sqrt{a^2 + b^2}\n", |
| 250 | + "$$\n" |
| 251 | + ] |
| 252 | + }, |
| 253 | + { |
| 254 | + "cell_type": "markdown", |
| 255 | + "id": "72997fa1-e58d-45e7-88e7-d295d9723d48", |
| 256 | + "metadata": {}, |
| 257 | + "source": [ |
| 258 | + "# Are There Restrictions Before $R^2 = a^2 + b^2$?\n", |
| 259 | + "\n", |
| 260 | + "Before the step $R^2 = a^2 + b^2$, there is no inherent restriction that forces $R$ to be positive. The square root function $\\sqrt{a^2 + b^2}$ is defined as the **non-negative root**, but the $\\pm$ arises because squaring both sides of an equation introduces an inherent ambiguity." |
| 261 | + ] |
| 262 | + }, |
| 263 | + { |
| 264 | + "cell_type": "markdown", |
| 265 | + "id": "d6cb31a9-f27c-4266-89c5-14470e5d8c7d", |
| 266 | + "metadata": {}, |
| 267 | + "source": [ |
| 268 | + "# Resolving the Ambiguity in $R$\n", |
| 269 | + "\n", |
| 270 | + "Notice that we still have ambiguity at $R$, where we can only choose one answer or the other. But let’s dig further:\n", |
| 271 | + "\n", |
| 272 | + "$$\n", |
| 273 | + "R = \\pm\\sqrt{a^2 + b^2}.\n", |
| 274 | + "$$\n", |
| 275 | + "\n", |
| 276 | + "Substituting both cases into our unified equation, we get:\n", |
| 277 | + "\n", |
| 278 | + "$$\n", |
| 279 | + "R\\cos(A \\mp x) \\quad \\text{ and } \\quad -R\\cos(A \\mp x).\n", |
| 280 | + "$$\n", |
| 281 | + "\n", |
| 282 | + "Zooming in on the second case, we can distribute the negative sign on $\\cos$:\n", |
| 283 | + "\n", |
| 284 | + "$$\n", |
| 285 | + "-R\\cos(A \\mp x) = R \\cdot -\\cos(A \\mp x)\n", |
| 286 | + "$$\n", |
| 287 | + "\n", |
| 288 | + "Using the trigonometric identity:\n", |
| 289 | + "\n", |
| 290 | + "$$\n", |
| 291 | + "-\\cos(\\theta) = \\cos(\\theta + \\pi)\n", |
| 292 | + "$$\n", |
| 293 | + "\n", |
| 294 | + "We can rewrite this as:\n", |
| 295 | + "\n", |
| 296 | + "$$\n", |
| 297 | + "R \\cdot -\\cos(A \\mp x) = R \\cos(A \\mp x + \\pi).\n", |
| 298 | + "$$\n", |
| 299 | + "\n", |
| 300 | + "$$\n", |
| 301 | + "R \\cdot -\\cos(A \\mp x) = R \\cos((A + \\pi) \\mp x).\n", |
| 302 | + "$$\n", |
| 303 | + "\n", |
| 304 | + "Now notice that $A$ has a period of $\\pi$, meaning:\n", |
| 305 | + "\n", |
| 306 | + "$$\n", |
| 307 | + "A + \\pi \\quad \\text{is functionally equivalent to} \\quad A.\n", |
| 308 | + "$$\n", |
| 309 | + "\n", |
| 310 | + "And thus\n", |
| 311 | + "\n", |
| 312 | + "$$\n", |
| 313 | + "R\\cos(A \\mp x + \\pi) = R\\cos(A \\mp x).\n", |
| 314 | + "$$\n", |
| 315 | + "\n", |
| 316 | + "We have rephrased the form with negative R, into the form with positive R\n", |
| 317 | + "- Hence, we can always take just the positive part of R\n", |
| 318 | + "\n", |
| 319 | + "$$\n", |
| 320 | + "\\boxed{\n", |
| 321 | + " R = \\sqrt{a^2 + b^2}\n", |
| 322 | + "}\n", |
| 323 | + "$$" |
| 324 | + ] |
| 325 | + }, |
| 326 | + { |
| 327 | + "cell_type": "markdown", |
| 328 | + "id": "7e70ea64-b61f-49e0-878d-655dbc539641", |
| 329 | + "metadata": {}, |
| 330 | + "source": [ |
| 331 | + "# Final Formula\n", |
| 332 | + "\n", |
| 333 | + "Thus, the R-formula for $a\\cos(x) \\pm b\\sin(x)$ is:\n", |
| 334 | + "\n", |
| 335 | + "$$\n", |
| 336 | + "a\\cos(x) \\pm b\\sin(x) = R\\cos(A \\mp x)\n", |
| 337 | + "$$\n", |
| 338 | + "\n", |
| 339 | + "where:\n", |
| 340 | + "\n", |
| 341 | + "$$\n", |
| 342 | + "A = \\arctan\\left(\\frac{b}{a}\\right), \\quad R = \\sqrt{a^2 + b^2}\n", |
| 343 | + "$$\n" |
| 344 | + ] |
| 345 | + }, |
| 346 | + { |
| 347 | + "cell_type": "markdown", |
| 348 | + "id": "5e1b6cc7-fdd7-489a-b854-ef1e9e5a524c", |
| 349 | + "metadata": {}, |
| 350 | + "source": [ |
| 351 | + "---\n", |
| 352 | + "### We can use the same logic to set up $a\\sin(x) \\pm b\\cos(x)$\n", |
| 353 | + "---" |
| 354 | + ] |
| 355 | + } |
| 356 | + ], |
| 357 | + "metadata": { |
| 358 | + "kernelspec": { |
| 359 | + "display_name": "Python 3 (ipykernel)", |
| 360 | + "language": "python", |
| 361 | + "name": "python3" |
| 362 | + }, |
| 363 | + "language_info": { |
| 364 | + "codemirror_mode": { |
| 365 | + "name": "ipython", |
| 366 | + "version": 3 |
| 367 | + }, |
| 368 | + "file_extension": ".py", |
| 369 | + "mimetype": "text/x-python", |
| 370 | + "name": "python", |
| 371 | + "nbconvert_exporter": "python", |
| 372 | + "pygments_lexer": "ipython3", |
| 373 | + "version": "3.12.9" |
| 374 | + } |
| 375 | + }, |
| 376 | + "nbformat": 4, |
| 377 | + "nbformat_minor": 5 |
| 378 | +} |
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