Table 2 Experimental conditions for the study of different particle flows.
Flow rate \(\left[\frac{\upmu\text{L}}{\text{min}}\right]\) | Mean velocity \(\left[\frac{\text{m}}{\textrm{s}}\right]\) | Channel’s Re number \(\left(R{e}_{c}\right)\) | Dean number \(\left(De\right)\) | Particle’s Re number \((R{e}_{p})\) | |||||
|---|---|---|---|---|---|---|---|---|---|
\({a}_{p}=1\) μm | \({a}_{p}=2.45\) μm | \({a}_{p}=4.16\) μm | \({a}_{p}=5.9\) μm | \({a}_{p}=8\) μm | \({a}_{p}=12\) μm | ||||
\(50\) | \(0.0868\) | \(6.7188\) | \(4.2118\) | \(0.0011\) | \(0.0067\) | \(0.0194\) | \(0.0390\) | \(0.0718\) | \(0.1615\) |
\(100\) | \(0.1736\) | \(13.4375\) | \(8.4235\) | \(0.0022\) | \(0.0135\) | \(0.0388\) | \(0.0781\) | \(0.1436\) | \(0.3230\) |
\(150\) | \(0.2604\) | \(20.1563\) | \(12.6353\) | \(0.0034\) | \(0.0202\) | \(0.0582\) | \(0.1171\) | \(0.2153\) | \(0.4845\) |
\(200\) | \(0.3472\) | \(26.8750\) | \(16.8470\) | \(0.0045\) | \(0.0269\) | \(0.0776\) | \(0.1562\) | \(0.2871\) | \(0.6460\) |
\(250\) | \(0.4340\) | \(33.5938\) | \(21.0588\) | \(0.0056\) | \(0.0337\) | \(0.0970\) | \(0.1952\) | \(0.3589\) | \(0.8075\) |
\(300\) | \(0.5208\) | \(40.3125\) | \(25.2705\) | \(0.0067\) | \(0.0404\) | \(0.1165\) | \(0.2342\) | \(0.4307\) | \(0.9690\) |
\(350\) | \(0.6076\) | \(47.0313\) | \(29.4823\) | \(0.0079\) | \(0.0471\) | \(0.1359\) | \(0.2733\) | \(0.5024\) | \(1.1305\) |
\(400\) | \(0.6944\) | \(53.7500\) | \(33.6940\) | \(0.0090\) | \(0.0539\) | \(0.1553\) | \(0.3123\) | \(0.5742\) | \(1.2920\) |
\(450\) | \(0.7813\) | \(60.4688\) | \(37.9058\) | \(0.0101\) | \(0.0606\) | \(0.1747\) | \(0.3514\) | \(0.6460\) | \(1.4535\) |
\(500\) | \(0.8681\) | \(67.1875\) | \(42.1175\) | \(0.0112\) | \(0.0673\) | \(0.1941\) | \(0.3904\) | \(0.7178\) | \(1.6150\) |
\(550\) | \(0.9549\) | \(73.9063\) | \(46.3293\) | \(0.0123\) | \(0.0741\) | \(0.2135\) | \(0.4294\) | \(0.7895\) | \(1.7765\) |
\(600\) | \(1.0417\) | \(80.6250\) | \(50.5410\) | \(0.0135\) | \(0.0808\) | \(0.2329\) | \(0.4685\) | \(0.8613\) | \(1.9380\) |
\(650\) | \(1.1285\) | \(87.3438\) | \(54.7528\) | \(0.0146\) | \(0.0875\) | \(0.2523\) | \(0.5075\) | \(0.9331\) | \(2.0995\) |
\(700\) | \(1.2153\) | \(94.0625\) | \(58.9646\) | \(0.0157\) | \(0.0942\) | \(0.2717\) | \(0.5466\) | \(1.0049\) | \(2.2610\) |
\(750\) | \(1.3021\) | \(100.7813\) | \(63.1763\) | \(0.0168\) | \(0.1010\) | \(0.2911\) | \(0.5856\) | \(1.0767\) | \(2.4225\) |
\(800\) | \(1.3889\) | \(107.5000\) | \(67.3881\) | \(0.0179\) | \(0.1077\) | \(0.3105\) | \(0.6246\) | \(1.1484\) | \(2.5840\) |
