laporan mekanika fluida h-02

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 FLUID MECHANICS AND HYDRAULIC EXPERIMENTAL REPORT MODULE H-02 HYDROSTATIC PRESSURE GROUP 22 Daniel Andiga Wibisana 1306437076 John William Horasia 1306437082 Raihan Alisha Nabila 1306437126 Fikri Dwisatrio 1306437132 Sabrina Nurul Hidayah 1306437145   Name of Assistant : Victor Saragih Date of Experiment : October 3, 2014 Date of Approval : Score : Assistant’s Signature : LABORATORY OF HYDRAULIC, HYDROLOGY, AND RIVER CIVIL ENGINEERING DEPARTEMENT ENGINEERING FACULTY UNIVERSITAS INDONESIA DEPOK 2014

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8/10/2019 Laporan Mekanika Fluida H-02

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HYDROSTATIC PRESSURE

1. Objective

This experimental work is intended to determine a hydrostatic force magnitude on thevertical plane. As well as determining the correlation between water level and mass load

on the apparatus.

2.Basic Theory

Any object that is put in the water will experience pressure that is perpendicular with its

surface by ρ.g.h (ρ is the density of water).

The magnitude of compressive force on the flat areas is:

…………………………………………………………………………………………………………………... (1)

And the location of the working point from the water surface is:

cg

gccg

y.AI

y …………………………………………………………………. (2)

Where:

ρ = density of water g = gravitational acceleration

ycg = distance of plane’s center of gravity from water surface

A = area of plane

Icg = moment of inertia of the plane in respect to the horizontal axis that cut the p lane’s center of

gravity

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θ = angle of the plane to the water surface

Zcf = distance of force’s working point from water surface

For “partially submerged” condition, the equation used:

Picture1.Partially submerged condition

– ……………………………………………………... (3)

……………………………………………… (4)

For “fully submerged” condition, the equation used:

Picture 2.Fully submerged condition

– ………………………………………. (5)

……………………………………………………………….. (6)

m.g

b

yd

ar’

r

L

m.g

b

yd

ar’

r

L

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8. Sharp shaft/pivot

9. Adjustable counterbalance

10. Water surface’s scale

11. Rectangular surface area

12. Drain valve

13. Leveling feet

4.Procedure of Experiment

1. Measuring the length of a, L, d and b from the apparatus

2. Setting the leveling feet so that the container is completely flat

3. Putting the weight hanger in the end of scale’s arm

4. Setting the adjustable counterbalance until the scale’s arm returns to flat condition 5. Put the loads on the weight hanger

6. Closing the draining valve and filling the container with water little by little until the

scale’s arm returns flat

7. Recording the water level (y) in the appropriate column

8. Performing step 5-7 until the maximum water level reached

9. Reducing the loads according to the addition of loading before

10. Lowering the water level by opening the draining valve until the scale’s arm returns flat

11. Recording the water level (y) in the appropriate column

12. Performing step 9-11 until the minimum water level is reached

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5. Observation and Data Calculation

a = 10 cm

b = 7.5 cm

d = 10 cm

L = 27.5 cm

FILLING TANK DRAINING TANK

Mass (m)

(gram)

Height of Water (y)

(mm)

Mass (m)

(gram)

Height of Water (y)

(mm)

50 45 50 46

70 56 70 56

90 68 90 63

110 69 110 68

130 76 130 76

150 82 150 82

170 87 170 87

190 93 190 93

210 98 210 98

230 103 230 103

250 109 250 108

270 114 270 113

290 118 290 118

310 122 310 123

330 127 330 128350 133 350 133

370 137 370 137

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1. Prove equation (3) and (5) with equation (1) and (2)

Equation (3)

 ̅ ⁄

(⁄ )

,-

Equation (5)

 ̅ . /

./

{ }. /

. /

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Partially Submerged Experiment

Table 1. Regression Linear, relationship between

FILLING TANKDRAINING

TANKAverage

y (x) m/y 2(y) x2 y2 xyMass Heightof

water(cm)

Mass(g)

Heightof

water(cm)

M H(g)

50 4,6 50 4,6 50 4,6 4,6 2,36294896 21,16 5,583527789 10,86956522

70 5,6 70 5,6 70 5,6 5,6 2,232142857 31,36 4,982461735 12,5

90 6,3 90 6,3 90 6,3 6,3 2,267573696 39,69 5,141890467 14,28571429

110 6,9 110 6,8 110 6,85 6,85 2,344291118 46,9225 5,495700847 16,05839416

130 7,6 130 7,6 130 7,6 7,6 2,250692521 57,76 5,065616823 17,10526316

150 8,2 150 8,2 150 8,2 8,2 2,230814991 67,24 4,976535524 18,29268293

170 8,7 170 8,7 170 8,7 8,7 2,246003435 75,69 5,04453143 19,54022989

190 9,3 190 9,3 190 9,3 9,3 2,196785756 86,49 4,825867656 20,43010753

210 9,8 210 9,8 210 9,8 9,8 2,186588921 96,04 4,781171111 21,42857143

Σ 66,95 20,31784226 522,3525 45,89730338 150,5105286

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y= -0.02597x + 2.450

Relative Mistake

|| | |

|| | |

y = -0.026x + 2.4508R² = 0.5657

y = -0.045x + 2.727R² = 1

0

0.5

1

1.5

2

2.5

3

0 2 4 6 8 10 12

m / y 2 ( y )

Height of water (cm)

Grapg of y and m/y2Partially Submerged Experiment

m/y2

Theory

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F-Hydrostatic:

Table of Hydrostatic Pressure for “partially submerged

Graph of Hydrostatic Force (Partially Submerged)

0

0.02

0.04

0.06

0.08

0.1

0.12

0 1 2 3 4 5

H e i g h t o

f w a t e r

( m )

Hydrostatic Force (N)

Hydrostatic ForcePartially Submerged

MassHeight of Water

(m)F-Hydrostatic

50 0,046 1,03789870 0,056 1,53820890 0,063 1,9467945

110 0,0685 2,301548625130 0,076 2,833128150 0,082 3,298122170 0,087 3,7125945190 0,093 4,2423345210 0,098 4,710762

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Fully Submerged Experiment

Table 1. Regression Linear, relationship between

FILLING TANKDRAINING

TANK Average

x2 y2 xy

Mass Heightof

water(cm)

Mass(g)

Heightof

water(cm) M (y) H (x)(g)

230 10,3 230 10,3 230 10,3 106,09 52900 2369

250 10,9 250 10,8 250 10,85 117,7225 62500 2712,5

270 11,4 270 11,3 270 11,35 128,8225 72900 3064,5

290 11,8 290 11,8 290 11,8 139,24 84100 3422

310 12,2 310 12,3 310 12,25 150,0625 96100 3797,5

330 12,7 330 12,8 330 12,75 162,5625 108900 4207,5

350 13,3 350 13,3 350 13,3 176,89 122500 4655

370 13,7 370 13,7 370 13,7 187,69 136900 5069

Σ 2400 96,3 1169,08 736800 29297

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*+ *+

Relative Mistake || | |

|| | |

y = 40.655x - 189.38R² = 0.9994y = 40.909x - 181.82

R² = 1

0

100

200

300

400

500

0 5 10 15 20

M a s s

( g )

Height of water (cm)

Graph of h and mFully Submerged Experiment

M (y)

Theory

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F-Hydrostatic:

Table of Hydrostatic Pressure for “fully submerged”

Graph of Hydrostatic Force (Fully Submerged)

00.020.040.060.08

0.10.120.140.16

4 5 6 7 8 9

H e i g h t o

f w a t e r

( m )

Hydrostatic Force (N)

Hydrostatic ForceFully Submerged

Mass Height of

Water (m)

F. Hydrostatic

230 0,103 5,1993250 0,1085 5,73885270 0,1135 6,22935290 0,118 6,6708310 0,1225 7,11225330 0,1275 7,60275350 0,133 8,1423370 0,137 8,5347

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6. Analysis

i. Analysis of Experiment

The Hydrostatic Pressure experiment has the objective to determine the force of

hydrostatic of water and to also determine the relationship between the height of water

and the mass load on the hydrostatic pressure apparatus. First of all, students have to

prepare the instruments that will be used in the experiment by referring to the module.

The hydrostatic pressure apparatus, the weights, and water have to be prepared. Before

adding weights, the apparatus have to be calibrated by turning the adjustable

counterbalance until the position of the apparatus is balanced. The way the apparatus

works is, when the tank is filled with water, there will be force acting perpendicularly on

the vertical part of the apparatus. That is why the apparatus will go up and down when

water is added or drained.This experiment consists of filling and draining the water tank. Students must take

note of the dimensions of the apparatus; length of a, L, d and b. As students add loads on

the weight hanger at the end of the scale’s arm, water is then added until the scale’s arm

returns flat. The starting load of the experiment is 50 grams. More loads are added until it

reaches 370 grams and the loads are added by 20 grams each time. For every time the

loads are added, students must add water until the scale’s arm is flat or balanced, then

record the water level which is millimeter. Once the load reaches 370 grams, the loads

are then reduced until it reaches the original weight which is 50 grams. The removing of

weight is also done by taking 20 grams of loads at each time. The water level is then

recorded once the scale’s arm is flat or balanced, and in order to do that the water would

have to be drained from the tank. If the water level is too low, then more water can be

added to reach the balanced state. The process of filling and draining the tank is done to

obtain more accurate data from the experiment.

It is evident that water has force acting on the surface of the apparatus because

whenever water is added or drained, the apparatus would go up or down until it is

balanced again. For data calculation, it is divided into two sections; partially and fully

submerged. This is because there are 2 different formulas used partially and fully

submerged object. When the apparatus is fully submerged, the vertical surface

experiences forces perpendicularly, but there is also another force coming from the top of

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the apparatus because water has forces in all directions. The data will be processed using

linear regression, y = bx + a, where y is the hydrostatic force, b is the mass, x is the

height of water, and a is the deviation value. When a and b are determined using manual

calculations, they are then compared to the theoretical values. And from there the relative

mistakes are calculated to show how accurate our data and calculations are.

ii. Result Analysis

In this experiment, students must record the water level at which the scale’ s arm

is at a flat or balanced state. When loads are added or removed, the scale’s arm will not

be balanced. Water is added or drained from the tank to balance with the loads on the

weight hanger. The data is divided into 2 sections; partially and fully submerged.

Partially submerged is measured at the water level below 100 mm and loadings startingfrom 50 grams to 210 grams. For fully submerged it is measured above 100 mm and

loadings starting from 210 grams all the way to 370 grams. The values of a and b are

determined for both sections and then compared to the theoretical values. And it is clear

that there had been some errors during obtaining and calculating the data. To find a and b,

we used

For partially submerged experiment, we obtained y= -0.02597x + 2.450

( and ). We then used the equations

and to find the theoretical values and we end up with relative

mistake for a = 42.28% and b = 10.13%. The coefficient of correlation obtained is R 2 =

0.565, which means that the x and y are not closely related.

For fully submerged experiment, we obtained (

and ). We then used the equations

*+and to find the theoretical values and we end up with

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relative mistake for a = 5.29% and b = 8.12%. The coefficient of correlation obtained is

R 2 = 0.999, which means that the x and y are very closely related.

From data calculation, we also obtain the value of hydrostatic force at each of the

water level by using the formula

for partially submerged and

for fully submerged..

iii. Graphical Analysis

According to observation and data calculation using linear regression, students

obtained 2 graphs. One graph shows the relationship between water level (y) and m/y 2 for

partially submerged experiment. The second graph shows the relationship between water

level and mass of the fully submerged experiment. For the partially submerged

experiment, the data of the graph is scattered and does not form a linear line because they

do not lie on the trend line. But for the fully submerged experiment, the graph forms a

linear line, which means that the relative mistake is low. The relationship between mass

and water level shows a directly proportional relationship, where if mass is removed, then

the water would also have to be removed. This is because as the water is reduced, the

hydrostatic force decreases.

What we also found for partially and fully submerged condition is that as the

water level increases, the hydrostatic force also increases. The graph shows a linearrelationship. It is evident that the hydrostatic force is directly proportional to the water

level of the object.

iv. Error Analysis

During this hydrostatic pressure experiment, there will be some mistakes or errors

that can occur. These errors will affect the data that will be collected and the

measurements that follow. This is evidence because the relative mistakes for a and b for

both partially and fully submerged are not equal to zero. These errors could be caused by

several factors

Inaccurate readings of the scale’s arm, where the balanced state is not

recorded accurately

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Inaccurate readings of the water level on the water tank could also hapen,

where the water level during filling and draining shows two different

numbers.

The eye posistion of the reader or observer that is not straight with the

scale’s arm or the water tank could also results in some mistakes in the

data recorded

There could also be some errors in the rounding of the numbers during the

calculation process

7. Conclusion

1. The value of hydrostatic force can be determined experimentally. The magnitude of

hydrostatic force is perpendicular to the surface of the apparatus. As more volume of the

object is submerged, the more hydrostatic force will act on it.

2. As the weight of the load increases, the height of the water also increases because more

water is needed to balance the scale’s arm.

3. The values of a and b obtained from experiment and theory show a linear relationship

between the relationship of mass and water level.

4. The weights that are added to the apparatus are able to be balanced by adding water to the

tank because there is hydrostatic force acting on the vertical surface of the apparatus.5. The sum of moments and hydrostatic force acting on the surfaces that are not vertical is

zero because the directions point straight to the hinge. The force is zero because it is not

perpendicular and these forces can be ignored during the experiment.

6. Relationship between h and m/h 2 is inversely proportional because as y increases, m/h 2

decreases.

7. Relationship between m and h is directly proportional because as y increases, h also

increases.

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8. References

Departemen Teknik Sipil Fakultas Teknik Universitas Indonesia. Modul Praktikum

Mekanika Fluida dan Hidrolika. Depok: Laboratorium Hidrolika, Hidrologi, dan

Sungai, 2013.

Potter, Merle C., David C. Wiggert, Bassem H. Ramadan, and Tom I-P.Shih. Mechanics

of Fluids . 4th ed. Englewood Cliffs, NJ: Prentice Hall, 1991. Print.

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