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Lab2 Dayli

The document presents experimental data on flow rates (Qc) and corresponding measurements of height (h1), volume (Vol), and pressure (p1) across various time intervals. It includes equations for predicting h1 based on Q, with high correlation coefficients indicating strong relationships. Additionally, it compares different flow rates from various sources, highlighting their theoretical and experimental values.

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didietmaluff
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2 views6 pages

Lab2 Dayli

The document presents experimental data on flow rates (Qc) and corresponding measurements of height (h1), volume (Vol), and pressure (p1) across various time intervals. It includes equations for predicting h1 based on Q, with high correlation coefficients indicating strong relationships. Additionally, it compares different flow rates from various sources, highlighting their theoretical and experimental values.

Uploaded by

didietmaluff
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as XLSX, PDF, TXT or read online on Scribd
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t(s) y1(m) Vol(m3) p1(m) Qc(lab) (m3/s) h1(lab) (m)

40.56 0.5911 1.2 0.45 0.0296 0.1411


51.51 0.5697 1.2 0.45 0.0233 0.1197
71.59 0.5462 1.2 0.45 0.0168 0.0962
117.19 0.5191 1.2 0.45 0.0102 0.0691
323.94 0.4851 1.2 0.45 0.0037 0.0351

h1(m) - Q(m3/s)
0.1600
0.1400
f(x) = 1.48228236454882 x^0.668826548379111
0.1200 R² = 0.999987738744278 Q(labor...
0.1000
h (m)

0.0800
0.0600
0.0400
0.0200
0.0000
0.0000 0.0050 0.0100 0.0150 0.0200 0.0250 0.0300 0.0350
Q (m3/s)

e (%) - h1
0.300

0.250

0.200

0.150
e (%)

0.100

0.050

0.000
0.0200 0.0400 0.0600 0.0800 0.1000 0.1200 0.1400 0.1600
h1 (m)
Qt(m3/s) u h1=1.4823Q^0.6688 error(%) h1/p1 h1/Tp1 kh(m)
0.0514 0.576 0.1407 0.260 0.314 0.157 0.00058
0.0396 0.588 0.1199 0.204 0.266 0.133 0.00058
0.0281 0.596 0.0962 0.044 0.214 0.107 0.00058
0.0168 0.608 0.0692 0.171 0.154 0.077 0.00058
0.0060 0.621 0.0351 0.095 0.078 0.039 0.00058

u - h1(m)
0.630
0.620
f(x) = − 1405.64690696219 x⁴ + 493.16184914769 x³ − 61.1000297145376 x² + 2.7050724280608 x + 0.58247782821758
0.610 h1 - Q. general
0.600
0.1600
0.590
0.1400
u

0.580
0.1200
0.570
0.1000
0.560
h1 (m)

0.0800
0.550
0.0600
0.0200 0.0400 0.0600 0.0800 0.1000 0.1200 0.1400 0.1600
0.0400 h1 (m)
0.0200
0.0000
0.0000 0.0020 0.0040 0.0060 0.0080 0.0100 0.0120
Q (m3/s)
h1 - Q
0.1600
0.1400
0.1200 Q (laboratorio)
0.1000 Q (Cipolleti)
Q (Balloffet)
h1 (m)

0.0800
Q (general)
0.0600
0.0400
0.0200
0.0000
0.0000 0.0050 0.0100 0.0150 0.0200 0.0250 0.0300 0.0350
Q (m3/s)

h1 - Q teórico
0.1600
0.1400
f(x) = 0.965045398158457 x^0.646441425981517
0.1200 R² = 0.999965888440079
0.1000
h1 (m)

0.0800
0.0600
0.0400
h1 - Q teórico
0.1600
0.1400
f(x) = 0.965045398158457 x^0.646441425981517
0.1200 R² = 0.999965888440079
0.1000

h1 (m)
0.0800
0.0600
0.0400
0.0200
0.0000
0.0000 0.0100 0.0200 0.0300 0.0400 0.0500 0.0600
Q (m3/s)
Ce Q kinsv y Carter (m3/s) L tan (cita/2) H1 Cv Cd Q(Cipolleti)
0.584 0.0104 0.3 0.25 0.1414513 1.004 0.63 0.0297
0.583 0.0069 0.3 0.25 0.1199568 1.003 0.63 0.0232
0.582 0.0040 0.3 0.25 0.0963654 1.003 0.63 0.0167
0.580 0.0018 0.3 0.25 0.0691859 1.002 0.63 0.0102
0.579 0.0003 0.3 0.25 0.0351221 1.001 0.63 0.0037

H/B
0.63 0.0348
0.63 0.0266
x + 0.58247782821758
0.63 0.0187
0.63 0.011
0.63 0.0038

0.1400 0.1600

h1 (m) - Q.Cipolleti (m3/s)


0.1600
0.1400
f(x) = 1.46725639042846 x^0.665794924872511
0.1200 R² = 0.999999937961677
0.1000
h (m)

0.0800
Q (laboratorio) 0.0600
Q (Cipolleti) 0.0400
Q (Balloffet) 0.0200
Q (general) 0.0000
0.0000 0.0050 0.0100 0.0150 0.0200 0.0250 0.0300 0.0350
Q (m3/s)

h1 (m) - Q. Balloffet (m3/s)


0.1600
0.1400
f(x) = 1.38401772951865 x^0.649668994176248
0.1200 R² = 0.999997876884756
0.1000
h (m)

0.0800
0.0600
0.0400
0.1600
0.1400
f(x) = 1.38401772951865 x^0.649668994176248
0.1200 R² = 0.999997876884756
0.1000

h (m)
0.0800
0.0600
0.0400
0.0200
0.0000
0.0000 0.0050 0.0100 0.0150 0.0200 0.0250 0.0300 0.0350
Q (m3/s)
2*h1 Balloffet Q general
0.2822 0.0298 0.0100
0.2394 0.0231 0.0078
0.1924 0.0165 0.0056
0.1382 0.0099 0.0034
0.0702 0.0035 0.0012

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