The Investigation of MHD Williamson Nanofluid over Stretching Cylinder with the Effect of Activation Energy

<div>The graph of concentration for different values of fitted rate constant (<span class="nowrap"><svg height="6.1673pt" id="M85" style="vertical-align:-0.2063904pt" version="1.1" viewbox="-0.0498162 -5.96091 5.50181 6.1673" width="5.50181pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M391 364C391 409 353 448 295 448C249 448 198 426 152 393C65 331 23 225 23 139C23 14 96 -12 146 -12C198 -12 280 9 367 101L351 124C300 78 242 48 194 48C129 48 109 107 109 162V191C208 213 391 266 391 364ZM313 350C313 305 268 261 113 223C132 334 187 381 217 398C227 404 244 405 261 405C290 405 313 385 313 350Z"></path></g></svg>)</span> and concentration exponent <span class="nowrap"><svg height="8.11156pt" id="M86" style="vertical-align:-2.15065pt" version="1.1" viewbox="-0.0498162 -5.96091 5.41045 8.11156" width="5.41045pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M384 393C384 425 346 448 294 448C244 448 200 431 150 399C75 351 23 271 23 176C23 90 52 45 132 19C150 13 166 9 195 2C245 -10 260 -27 260 -55C260 -92 234 -127 218 -145L237 -159C271 -137 333 -93 333 -18C333 43 283 62 228 74C199 80 186 84 172 89C116 109 101 150 101 210C101 318 164 400 241 400C276 400 301 390 327 356C334 347 338 343 346 345C367 349 384 374 384 393Z"></path></g></svg>.</span></div>

Advances in Mathematical Physics

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Figure 13

Figure 13: The Investigation of MHD Williamson Nanofluid over Stretching Cylinder with the Effect of Activation Energy 