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Assignment 2 Fluid particles and processes

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CURTIN UNIVERSITY OF TECHNOLOGY 2015 0 Table of Contents Question 1 ..................................................................................................................................................... 1 Question 2 ..................................................................................................................................................... 7 Question 3 ................................................................................................................................................... 14 Question 4 ................................................................................................................................................... 16 Question 5 ................................................................................................................................................... 21 References .................................................................................................................................................. 24 Appendix. .................................................................................................................................................... 25 Appendix question 4 ............................................................................................................................... 25 Table of figures Table 2 1 Filtrate volume over time .............................................................................................................. 7 Table 2 2 Basic data for calculation used in question 2 ................................................................................ 7 Table 2 3 Calculated values for the plotting of B vs t/B ................................................................................ 9 Table 4 1 Time and interface height for tank thickener 16 Table 4 2 Tabulated and calculated values for height vs time.................................................................... 18 Table 4 3 Tangent lines generated with Matlab 2nd m-file (Martina and Delli 2009) ............................... 20 Graph 2 1 t/b vs b to find alpha and betta for resistance calculation ........................................................ 13 Graph 4 1 H vs T graph ................................................................................................................................ 19
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Page 1: Assignment 2 Fluid particles and processes

CURTIN UNIVERSITY OF TECHNOLOGY 2015 0

Table of Contents Question 1 ..................................................................................................................................................... 1

Question 2 ..................................................................................................................................................... 7

Question 3 ................................................................................................................................................... 14

Question 4 ................................................................................................................................................... 16

Question 5 ................................................................................................................................................... 21

References .................................................................................................................................................. 24

Appendix. .................................................................................................................................................... 25

Appendix question 4 ............................................................................................................................... 25

Table of figures Table 2 1 Filtrate volume over time .............................................................................................................. 7

Table 2 2 Basic data for calculation used in question 2 ................................................................................ 7

Table 2 3 Calculated values for the plotting of B vs t/B ................................................................................ 9

Table 4 1 Time and interface height for tank thickener 16

Table 4 2 Tabulated and calculated values for height vs time .................................................................... 18

Table 4 3 Tangent lines generated with Matlab 2nd m-file (Martina and Delli 2009) ............................... 20

Graph 2 1 t/b vs b to find alpha and betta for resistance calculation ........................................................ 13

Graph 4 1 H vs T graph ................................................................................................................................ 19

Page 2: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 1

Question 1

Oxygen is supplied to an astronaut through an umbilical hose that is 7 m long. The pressure in

the oxygen tank is 200 kPa at a temperature of 10 ΒΊC, and the pressure in the space suit is 20 kPa. If

the umbilical hose has an equivalent roughness of 0.01 mm, what should the hose diameter be to supply

oxygen at a rate of 0.05 kg/s?

The general assumptions:

o The flow is taken to be under isothermal condition

o Behaviour of oxygen as an ideal gas.

o Pipe length is assumed long, hence average density is taken for calculation

First, calculate the upstream (𝜌 1) and downstream (𝜌2) density:

Upstream pressure: 200 kPaβ‰ˆ 200 Γ— 103π‘ƒπ‘Ž

Molecular weight of oxygen, Mw: 32 g/mol

The ideal gas law is used to calculate the density:

𝜌 =𝑃𝑀

𝑅𝑇

1.1

𝜌1 =π‘ƒπ‘’π‘π‘ π‘‘π‘Ÿπ‘’π‘Žπ‘šπ‘€π‘€

𝑅𝑇=

200 Γ— 103(32

1000)

8.314(10 + 273.15)= 𝟐. πŸ•πŸ π’Œπ’ˆ/π’ŽπŸ‘

𝜌2 =π‘ƒπ‘‘π‘œπ‘€π‘›π‘ π‘‘π‘Ÿπ‘’π‘Žπ‘šπ‘€π‘€

𝑅𝑇=

20 Γ— 103(32

1000)

8.314(10 + 273.15)= 𝟎. πŸπŸ•πŸ π’Œπ’ˆ/π’ŽπŸ‘

οΏ½Μ…οΏ½ =𝜌1 + 𝜌2

2=

2.7187 + 0.2719

2= 𝟏. πŸ’πŸ—πŸ” π’Œπ’ˆ/π’ŽπŸ‘

Page 3: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 2

As velocity is not given, it needs to be substituted.

οΏ½Μ‡οΏ½ = πœŒπ‘£π΄

1.2

𝑣 =οΏ½Μ‡οΏ½

�̅�𝐴

𝑠𝑒𝑏𝑠𝑑𝑖𝑑𝑒𝑑𝑖𝑛𝑔 π‘£π‘Žπ‘™π‘’π‘’ 𝑖𝑛 ∢ 𝑣 = 0.0234

𝐷2

The isothermal equation is:

(𝑃12 βˆ’ 𝑃2

2) = π‘“πœŒ1𝑣2𝑋𝑃1

𝐷

1.3

Substituting value in, we will obtain:

(2000002 βˆ’ 200002) = 𝑓 Γ— 2.72 Γ— (0.0234

𝐷2)2 Γ— 7 Γ— 200000 Γ—

1

𝐷

𝐷 = 0.035(𝑓)1/5

Where D = diameter of pipe, X = length of pipe and f = friction factor.

Reynolds number equation is:

𝑅𝑒 =πœŒπ‘’π‘π‘ π‘‘π‘Ÿπ‘’π‘Žπ‘šπ‘£π·

πœ‡=

3230.9

𝐷

The viscosity of oxygen , πœ‡ = 1.995 Γ— 10βˆ’5 π‘ƒπ‘Ž. 𝑠(The Engineering Toolbox n.d).

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ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 3

Iteration 1: By assuming f= 0.01:

Substitute the variables inside to find diameter first:

𝐷 = 0.035(0.01)1/5 = 0.0139π‘š

Then, use the calculated D to find the Reynolds number:

𝑅𝑒 =3230.9

0.0139= 232438.8

πœ€

𝐷= 0.000719

𝑓 = 0.0198

Iteration 2: f=0.0198:

𝐷 = 0.035(0.0198)1/5 = 0.01597π‘š

𝑅𝑒 =3230.9

0.01597= 202265.8

πœ€

𝐷= 0.0005

𝑓 = 0.0189

Iteration 3: f=0.0189:

𝐷 = 0.035(0.0189)1/5 = 0.0158π‘š

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ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 4

𝑅𝑒 =3230.9

0.0158= 204156.5

πœ€

𝐷= 0.00053

𝑓 = 0.0189

Since the difference between the friction factor is insignificant, f = 0.0189 is acceptable.

Thus, the diameter of the umbilical hose = 0.0158m.

Checking the magnitudes of the terms:

𝐺 =π‘š

𝐴= 255 π‘˜π‘”/π‘š2𝑠

Term 1:

𝐺2𝑙𝑛 (𝜌1

𝜌2) = 2552 Γ— 𝑙𝑛 (

2.72

0.272) = 199725

Term 2:

οΏ½Μ…οΏ½(𝑃2 βˆ’ 𝑃1) = 1.496 Γ— (20,000 βˆ’ 200,000) = βˆ’269280

Term 3:

𝑓𝐺2𝑋

2𝐷=

0.0189 Γ— 2552 Γ— 7

2 Γ— 0.158= 272240.7

Term 1 (kinetic energy term) is not negligible; therefore it needed to be considered in calculating the

diameter of the umbilical hose.

Page 6: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 5

The general equation for isothermal flow is shown as:

𝐺2𝑙𝑛 (𝜌1

𝜌2) + οΏ½Μ…οΏ½(𝑃2 βˆ’ 𝑃1) +

𝑓𝐺2𝑋

2𝐷= 0

It is known that 𝜌1

𝜌2=

𝑃1

𝑃2:

𝐺2𝑙𝑛 (𝑃1

𝑃2) +

𝑀𝑀

2𝑅𝑇(𝑃2

2 βˆ’ 𝑃12) +

𝑓𝐺2𝑋

2𝐷= 0

(πœŒπ‘£)2𝑙𝑛 (𝑃1

𝑃2) +

𝑀𝑀

2𝑅𝑇(𝑃2

2 βˆ’ 𝑃12) +

𝑓𝐺2𝑋

2𝐷= 0

After substituting value:

(9.33 Γ— 10βˆ’3 Γ— 𝐷) βˆ’ (269289 Γ— 𝐷5) + 0.014175 Γ— 𝑓 = 0

1st iteration, f = 0.0189

(9.33 Γ— 10βˆ’3 Γ— 𝐷) βˆ’ (269289 Γ— 𝐷5) + 0.000268 = 0

After using try and error method, we obtain:

𝐷 = 0.0174 π‘š

𝑅𝑒 =3230.9

0.0174= 185683.9

πœ€

𝐷= 0.000575

𝑓 = 0.01932

2nd iteration, f = 0.01932

(9.33 Γ— 10βˆ’3 Γ— 𝐷) βˆ’ (269289 Γ— 𝐷5) + 0.000274 = 0

𝐷 = 0.0174 π‘š

𝑅𝑒 =3230.9

0.0174= 185684

Page 7: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 6

πœ€

𝐷= 0.00055

𝑓 = 0.0193

Since the difference between f is insignificant, D = 0.0174 m.

Page 8: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 7

Question 2

A filter press with a plate area of 1.5 m2 operates at a constant differential pressure of 330 kPa is

fed with a slurry of 16.5 mass percent CaCO3 in water.

Filtrate volume x103 4 6.1 7.7 9.65 11.47 13.6 15.5

Time(min) 10 20 30 45 60 80 100 Table 2 1 Filtrate volume over time

i) Estimate the individual resistance of the cake and filter medium and also the total combined specific resistance of the filtration equipment.

Data Given:

CaCO3 slurry feed Filter aid

Solid density 2700 kg/m3 -

Feed solid loading 50 kg/m3 -

Filtrate viscosity 10 cP -

Sphericity 0.9 0.7

Average particle size 3.33mm 1mm

Porosity 0.25 0.75 Table 2 2 Basic data for calculation used in question 2

Question:

- Resistance of the cake and the combine resistance of the filter medium and equipment

Assumptions:

Initial filtrate volume, π΅π‘œ = 0

Initial time, π‘‘π‘œ = 0

Answer:

Area=1.5m2

Constant pressure: 330π‘˜π‘ƒπ‘Ž Γ— 103 = 330000π‘ƒπ‘Ž

Filter aid=medium

Slurry feed=cake

Page 9: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 8

Slurry of 16.5% kg CaCO3 in water.

𝑋 = (30|1π‘š

100π‘π‘š Γ— 20) = 6π‘š

Step 1: Volume fraction of solids

𝒄 =π’Ž

𝝆𝒔

4.1

50

2700= 0.0185 β‰ͺ 1

For filter aid, specific surface 𝑺𝒇

𝑆𝑓 =6

βˆ…π·

4.2

6

0.75 Γ— 1 Γ— 10βˆ’3= 8000π‘š2π‘šβˆ’3

Since constant βˆ†π‘ƒ; the values of the resistance 𝛼 π‘Žπ‘›π‘‘ 𝛽 can be found from a t/B vs. B graph. The

graph is plotted from the values in table 2.3. Graph 2.2 shows the plotted values. A line if best fit

is drawn. The equation for the linear line was determined to be:

𝑦 = 22.8π‘₯ + 57.9 4.3

The following equation is to be used to solve this problem:

βˆ†π‘ƒ(𝑑 βˆ’ 𝑑0) =πœ‡π‘šπ‘ π›Ό

2𝐴2(𝐡2 βˆ’ 𝐡0

2) +πœ‡

𝐴𝛽(𝐡 βˆ’ 𝐡0)

4.4

Since 𝐡0 and 𝑑0 are both equal to zero, the equation can be simplified as follow:

βˆ†π‘ƒπ‘‘ =πœ‡π‘šπ‘ π›Ό

2𝐴2𝐡2 +

πœ‡

𝐴𝛽𝐡

Page 10: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 9

𝑑

𝐡=

πœ‡π‘šπ‘ π›Ό

2𝐴2βˆ†π‘ƒπ΅ +

πœ‡

π΄βˆ†π‘ƒπ›½

Filtrate volume x103 dm3 4 6.1 7.7 9.65 11.47 13.6 15.5

Filtrate volume m3 (B) 4 6.1 7.7 9.65 11.47 13.6 15.5

Time(min) 10 20 30 45 60 80 100

Time(s) 600 1200 1800 2700 3600 4800 6000

t/B (s/m3) 150 196.7213 233.7662 279.7927 313.8622 352.9412 387.0968

Table 2 3 Calculated values for the plotting of B vs t/B

From the graph, it is obtained that the gradient of the line, m = 22.8 and the intercept = 57.9.

(i) Resistance of cake

πœ‡π‘šπ‘ π›Ό

2𝐴2βˆ†π‘ƒ= 22.8

∴ 𝛼 =(22.8)(2𝐴2βˆ†π‘ƒ)

πœ‡π‘šπ‘ =

22.8 Γ— 2 Γ— 1.52 Γ— 330 Γ— 103

0.001 Γ— 50

𝜢 = πŸ”. πŸ•πŸ• Γ— πŸπŸŽπŸ–π’Ž

π’Œπ’ˆ

(ii) Resistance of medium

πœ‡

π΄βˆ†π‘ƒπ›½ = 57.9

∴ 𝛽 =(57.9)(π΄βˆ†π‘ƒ)

πœ‡=

57.9 Γ— 330 Γ— 103 Γ— 1.5

0.001

𝜷 = 𝟐. πŸ–πŸ” Γ— πŸπŸŽπŸπŸŽπ’Žβˆ’πŸ

iii)Specific resistance of cake π’“π’Ž:

π’“π’Ž =𝛽

𝑋

4.5

π’“π’Ž =423.18 Γ— 106

6= πŸ•πŸŽ. πŸ“πŸ‘ Γ— πŸπŸŽπŸ”π’Žβˆ’πŸ

Page 11: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 10

iv)Specific resistance of cake, 𝒓𝒄

𝒓𝒄 = πœŒπ‘ (1 βˆ’ πœ€)𝛼 4.6

𝒓𝒄 = 2700(1 βˆ’ 0.25)(299.26 Γ— 103) = πŸ”πŸŽπŸ”. 𝟎 Γ— πŸπŸŽπŸ” π’Žβˆ’πŸ

Total specific resistance:

π’“π’Ž + 𝒓𝒄 = 70.53 Γ— 106π‘šβˆ’2 + 606.0 Γ— 106 π‘šβˆ’2 = πŸ’. πŸπŸ•πŸ’ Γ— πŸπŸŽπŸπŸ”π’Žβˆ’πŸ

2) For 75% slurry

Filtrate volume 𝑖𝑠 11.47 Γ— 103 π‘‘π‘š3 at 60 minutes.

1 π‘š3 = 1000 π‘‘π‘š3

∴ {1 π‘š3

1000 π‘‘π‘š3 |11.47 Γ— 103π‘‘π‘š3} = 11.47π‘š3

Total volume of cake is:

11.47

0.75= 15.29π‘š3

The volume of the filtrate is 11.47π‘š3 and a filter aid with the area of 3.82 π‘š2 are used.

Total surface area in cake:

(11.47 Γ— 2002) + (3.82 Γ— 8000) = 53522.94π‘š2

∴ 𝑆𝑝𝑒𝑐𝑖𝑓𝑖𝑐 π‘ π‘’π‘Ÿπ‘“π‘Žπ‘π‘’ π‘œπ‘“ π‘‘π‘œπ‘‘π‘Žπ‘™ π‘ π‘œπ‘™π‘–π‘‘π‘ , 𝑆 =𝐴

𝑉

53522.94

15.29= 3500.52π‘š2/π‘š3

Page 12: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 11

Average porosity= (0.75 Γ— 0.25) + (0.25 Γ— 0.7) = 0.3625

∴Total cake resistance:

(1 βˆ’ πœ€)2𝑆2

πœ€3

4.7

(1 βˆ’ 0.3625)23500.522

0.36253= 104.54 Γ— 106

∴Change of resistance:

15.29 Γ— 104.54 Γ— 106 = 1.69 Γ— 109

The factor for original resistance:

Equation 4.7 is reused

=(1 βˆ’ 0.25)220022

0.253

= 144.3 Γ— 106

Relative resistance:

𝟏. πŸ” Γ— πŸπŸŽπŸ—

πŸπŸ’πŸ’. πŸ‘ Γ— πŸπŸŽπŸ”= 𝟏𝟏. πŸŽπŸ—

Page 13: Assignment 2 Fluid particles and processes

CURTIN UNIVERSITY OF TECHNOLOGY 2015 0

Graph 2 1 t/b vs b to find alpha and betta for resistance calculation

Page 14: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 14

Question 3

Water percolates downwards through a san filter of thickness 15 mm, consisting of sand grains of

effective diameter 0.3 mm and void fraction 0.42. The depth of the effectively stagnant clear water above

the filter is 20 mm and the pressure at the base of the sand filter is atmospheric. Calculate the volumetric

flow rate per m2 of packed bed. Given fluid density and viscosity are 0.89x10-3 N s/m2 and 997 kg/m3

respectively.

Assumptions:

o Sand particles are taken as spherical in shape and hence the sphericity is 1.

o Kozeny constant is taken as 4.2 because the sand particles are assumed to be spherical in shape.

o Atmospheric pressure acts on the water surface.

o Flow of water through the sand filter is laminar.

Given Data:

Sand Feed (water) Diameter 0.3 mm - pressure 101325 Pa Height 15mm 20 mm Porosity 0.42 - Density - 997 kg/m3 viscosity - 0.89 x 10-3 Ns/m2 Ac

Solution:

Calculating the specific surface,

S = 6

πœ‘π· =

6

1 Γ— 0.3 Γ—10βˆ’3 = 20000 m2/m3

P1 = Pw+ PA is taken as the pressure at the bottom of the water level. The pressure equals to the

atmospheric pressure acting on the water surface and the pressure due to the water depth (pressure

head)

P2 = 101325 Pa is the pressure at the bottom of the sand filter.

Page 15: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 15

Pw = ρ𝑀.g.h = 997 x 9.81 x 20 x 10-3 = 195.6114

Ξ”P = P1 – P2 = (195.6114 + 101325) – 101325 = 195.6114 Pa (change in pressure is the pressure head)

Assuming the flow of water is laminar through the sand medium,

Application of Kozeny equation (K = 4.2),

βˆ’Ξ”P

Ξ”X =

πΎπ‘£πœ‡(1βˆ’πœ€2)𝑆2

πœ€3 = 4.2 .𝑣.(1βˆ’0.422)200002

0.423 (where Ξ”X = 15 Γ— 10βˆ’3 )

𝑣 =195.6114 Γ— 0.423

4.2 Γ— 0.89 Γ— 10βˆ’3 Γ— (1 βˆ’ 0.42)2 Γ— 200002 Γ— 15 Γ— 10βˆ’3

𝑣 = 0.00192 m/s (superficial fluid velocity)

Recheck the flow type using Reynolds number with the velocity value,

Calculating modified Reynolds number for porous flow through sand medium,

Re = 𝜌 𝑣𝑝𝐷𝐻

πœ‡

Actual velocity of fluid through the interstices vp,

vp = v/πœ€ = 0.00192/0.42 = 0.00457 m/s

Hydraulic diameter DH = πœ€

(1βˆ’πœ€)𝑆 =

0.42

(1βˆ’0.42) Γ—20000 = 3.6207 x 10-5 m

Hence, the modified Reynolds number calculation is performed,

Re = 𝜌 𝑣𝑝𝐷𝐻

πœ‡ =

997 Γ—0.00457 Γ— 3.6207 x 10βˆ’5

0.89 Γ—10βˆ’3

Re = 0.1853

This confirms the assumption of laminar flow since the modified Reynolds number is less than 2.

(Note: Turbulent flow for porous flow is for a modified Reynolds number value above 2)

Hence, the volumetric flowrate per m2 is taken from the superficial velocity v,

Q (volumetric flowrate m3/s)= vA

Q (volumetric flowrate per m2 = m/s) = v = 0.00192 m/s

Page 16: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 16

Question 4 A continuous cylindrical-tank thickener is to be designed to handle 5.5 x103 pounds of solids per

hour. The feed contains 0.035 mass fraction of limestone; the required underflow concentration is 0.21

mass fraction. Solid SG: 2.71 and solid size 5 ΞΌm. Estimate the minimum area of the thickener required

(base on 10 points plot). Data: batch settling test result collect is as follow:

Time(min) interface height(cm)

0 102.8

5 91.2

10 80.9

15 71.7

20 63.6

25 56.4

30 50.1

40 39.4

50 30.9

70 19.2

90 13.88

110 10.2

130 9.6

150 9.2 Table 4 1 Time and interface height for tank thickener

Given data:

Data Values

Mass of solid =5.5 Γ— 103 π‘π‘œπ‘’π‘›π‘‘π‘  π‘π‘’π‘Ÿ β„Žπ‘œπ‘’π‘Ÿ

Mass fraction of limestone =0.035

Underflow mass fraction =0.21

Mass fraction 𝐢𝐴𝐢𝑂3 =0.0291

Solid S.G. =2.71

Solid size(diameter) = 5 ΞΌm

Page 17: Assignment 2 Fluid particles and processes

ASSIGNMENT 2 CHEN3009 FLUID AND PARTICLE PROCESSES MIRI 05/25/2015

CURTIN UNIVERSITY OF TECHNOLOGY 2015 17

Method :

1. Convert all the mass fraction to volume fraction

2. Tabulate the table in order to get the πœ‘π‘šπ‘–π‘›

3. Get the area at πœ‘π‘šπ‘–π‘›

Assumptions:

1. Water and πΆπ‘ŽπΆπ‘‚3 is assumed to be one solution.

2. The minimum area is determined using πœ‘π‘šπ‘–π‘›

3. The specific gravity of the water is 1.

Convert all the mass fraction to volume fraction

π‘‰π‘œπ‘™π‘’π‘šπ‘’ π‘œπ‘“ πΆπ‘ŽπΆπ‘‚3 =0.0291

2.71= 0.010738 𝑙

π‘‰π‘œπ‘™π‘’π‘šπ‘’ π‘œπ‘“ π‘€π‘Žπ‘‘π‘’π‘Ÿ = (1 βˆ’ 0.0291)

1= 0.9709 𝑙

Volume fraction of C0 :

0.010738

0.010738 + 0.9709= 0.0109389

πΆπ‘œπ»π‘œ = 0.0109389 Γ— 102.8 = 1.1245

For underflow system

π‘‰π‘œπ‘™π‘’π‘šπ‘’ π‘œπ‘“ πΆπ‘ŽπΆπ‘‚3 =0.21

2.71= 0.0775 𝑙

π‘‰π‘œπ‘™π‘’π‘šπ‘’ π‘œπ‘“ π‘€π‘Žπ‘‘π‘’π‘Ÿ = (1 βˆ’ 0.21)

1= 0.79 𝑙

Volume fraction of 𝐢𝑂3 :

0.0775

0.0775 + 0.79= 0.0893

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The results and the graph were obtained by using MATLAB. Two m.files were used to plot the graph. The

procedure is outlined below

1) Graph of H vs T is plotted. The first m-file (h_vs_t.m) is utilized for these. Only the curve line is obtained.

2) The tangent of the lines to the time values are determined using a separate m-file (getthetangent.m)

(Martina and Delli 2009). The slope of the lines and the gradients are recorded as shown in Table 4.3. The

gradient and the intersections are converted to y=mx+c form.12 tangent lines are taken.

3) Modifications were done to the first m-file to display the tangent lines.

4) Results after tabulation in order to get the πœ‘π‘šπ‘–π‘›

H1 (cm) V (cm/min) Co Ho (cm) C=(CoHo)/H1 πœ‘π‘π‘Žπ‘‘π‘β„Ž 𝒄𝒖 𝒄𝒖

𝒄𝒖 βˆ’ 𝟏 πœ‘π‘ 

(kg/m2s)

102 2.19 0.010939 102.8 0.011025 0.024144 0.0893 1.140845 0.027545

100 1.95 0.010939 102.8 0.011245 0.021928 0.0893 1.144068 0.025087

97.7 1.73 0.010939 102.8 0.01151 0.019912 0.0893 1.147961 0.022858

94.2 1.53 0.010939 102.8 0.011938 0.018264 0.0893 1.154307 0.021083

90.2 1.35 0.010939 102.8 0.012467 0.01683 0.0893 1.16226 0.019561

86 1.2 0.010939 102.8 0.013076 0.015691 0.0893 1.171544 0.018383

77.8 0.96 0.010939 102.8 0.014454 0.013876 0.0893 1.193116 0.016555

69 0.762 0.010939 102.8 0.016297 0.012419 0.0893 1.223244 0.015191

49 0.426 0.010939 102.8 0.022949 0.009776 0.0893 1.34588 0.013158

34.1 0.225 0.010939 102.8 0.032977 0.00742 0.0893 1.585501 0.011764

22 0.107 0.010939 102.8 0.051114 0.005469 0.0893 2.338584 0.01279

12.9 0.025 0.010939 102.8 0.087172 0.002179 0.0893 41.96447 0.091453

Table 4 2 Tabulated and calculated values for height vs time

The formulas below were used to calculate the values above.

𝝋𝒃𝒂𝒕𝒄𝒉 = π‘ͺ Γ— 𝑽 4.1

𝝋𝒔 = 𝝋𝒃𝒂𝒕𝒄𝒉

𝒄𝒖

𝒄𝒖 βˆ’ 𝟏

4.2

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Graph 4 1 H vs T graph

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Tangent lines from MATLAB

y1 -2.19x+102

y2 -1.95x+100

y3 -1.73x+97.7

y4 -1.53x+94.2

y5 -1.35x+90.2

y6 -1.2x+86

y7 -0.96x+77.8

y8 -0.762x+69

y9 -0.426x+49

y10 -0.225x+34.1

y11 -0.107x+22

y12 -0.0s5x+12.9 Table 4 3 Tangent lines generated with Matlab 2nd m-file (Martina and Delli 2009)

The πœ‘π‘šπ‘–π‘›is calculated by first converting the mass flow rate to volumetric flow rate. The

calculation is then continued.

οΏ½Μ‡οΏ½ =5.5 Γ— 103π‘π‘œπ‘’π‘›π‘‘π‘ 

1 β„Žπ‘Ÿ|

1 β„Žπ‘Ÿ

60 π‘šπ‘–π‘›|

0.453592 π‘˜π‘”

1 π‘π‘œπ‘’π‘›π‘‘= 41.58 π‘˜π‘”/π‘šπ‘–π‘›

𝑄 =οΏ½Μ‡οΏ½

𝜌=

41.58 π‘˜π‘”/π‘šπ‘–π‘›

2710π‘˜π‘”π‘š3

= 0.0153π‘š3

π‘šπ‘–π‘›= 1.53

π‘π‘š3

π‘šπ‘–π‘›

The minimum area is then determined:

𝑄 = 𝐴. πœ‘π‘  4.3

𝐴 =1.53 Γ— 104 π‘π‘š3

π‘šπ‘–π‘›πŸŽ. πŸŽπŸπŸπŸ•πŸ”πŸ’ π‘π‘š/π‘šπ‘–π‘›

= πŸπŸ‘πŸŽπŸŽπŸ“πŸ•πŸ–π’„π’ŽπŸ = πŸπŸ‘πŸŽ. πŸŽπŸ”π’ŽπŸ

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Question 5

150 kg of uniform spherical particles with a diameter of 60 ΞΌm and particle density 2000

kg/m3 are fluidized by water (density 1000 kg/m3, viscosity 0.001 Pa s) in a circular bed of cross-

sectional area 0.5 m2. The voidage at incipient fluidization is known to be 0.47. Calculate:

a. the minimum fluidized velocity (m/min) and the bed height at incipient fluidization

b. the mean fluidized bed voidage and height when the liquid flow rate is 2.25x10-5 m3/s.

Slow flow is assumed.

𝑆 =6

𝐷

5.1

𝑆 =6

60 Γ— 10βˆ’6

𝑆 = 105

π‘‰π‘šπ‘“ =(πœŒπ‘  βˆ’ 𝜌)π‘”πœ€3

𝐾. πœ‡. (1 βˆ’ πœ€)𝑆2

5.2

π‘‰π‘šπ‘“ =(2000 βˆ’ 1000) Γ— 9.81 Γ— 0.473

4.2 Γ— 0.001 Γ— (1 βˆ’ 0.47)(105)2

π‘‰π‘šπ‘“ = 4.575 Γ— 10βˆ’5π‘š/𝑠

𝑅𝑒 =πœŒπ‘‰π‘šπ‘“π·

πœ‡

5.3

𝑅𝑒 =2000 Γ— 4.575 Γ— 10βˆ’5 Γ— 60 Γ— 10βˆ’6

0.001

𝑅𝑒 = 5.49 Γ— 10βˆ’3

πŸ“. πŸ’πŸ— Γ— πŸπŸŽβˆ’πŸ‘ < 𝟏.

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Assumption confirmed. Flow is slow

Bed height

𝑀𝐡 = (1 βˆ’ πœ€). πœŒπ‘ . 𝐴. 𝐻

5.4

150 = (1 βˆ’ 0.47). (2000). (0.5). 𝐻

𝑯 = 𝟎. πŸπŸ–πŸ‘πŸŽ π’Ž

Voidage; 𝑉𝑓

𝑉𝑓 =𝑄

𝐴

5.5

2.25 Γ— 10βˆ’5 π‘š3

𝑠

0.5 π‘š2= 4.5 Γ— 10βˆ’5

π‘š

𝑠

Find Vo

π‘‰π‘œ =𝐷2(πœŒπ‘  βˆ’ 𝜌)𝑔

18πœ‡

π‘‰π‘œ =(60 Γ— 10βˆ’6)2(2000 βˆ’ 1000)(9.81)

18(0.001)

π‘‰π‘œ = 1.962 Γ— 10βˆ’3 π‘š

𝑠

Find the voidage

Since Re< 0.3, The Richardson –Zaki equation is used, n=4.65

πœ€π‘› =𝑉𝑓

π‘‰π‘œ

5.6

πœ€ = βˆšπ‘‰π‘“

π‘‰π‘œ

𝑛

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πœ€ = √4.5 Γ— 10βˆ’5

1.962 Γ— 10βˆ’3

4.65

𝜺 = 𝟎. πŸ’πŸ’πŸ•πŸ

a. Find the Bed height. Reusing equation 5.4;

𝑀𝐡 = (1 βˆ’ πœ€). πœŒπ‘ . 𝐴. 𝐻

130 = (1 βˆ’ 𝟎. πŸ’πŸ’πŸ•πŸ). (2000). (0.5). 𝐻

𝑯 = 𝟎. πŸπŸ‘πŸ“πŸπ’Ž

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References Martina, Sandra, and Jean Luc Delli. 2009. Matlab License Universe Picarde Jules Verne. April. Accessed

May 23, 2015. https://www.u-picardie.fr/~dellis/Matlab_Licence/getthetangent.m.

Rhodes, Martin. 2008. Introduction to Particle Technology Second edition. England: John Wiley and Sons,

Ltd.

RICHARDSON, J. F., J. H. HARKER, and J. R. BACKHURST. 2002. "Chapter 16 Motions of Particle in a fluid."

In CHEMICAL ENGINEERING Volume 2 5th edition Particle technology and Separation Process,

146-187. Great Britian: Butterworth Heinemann.

Wischnewski, Berndt , and Bernhard Spang. n.d. CalcSteam.

http://www.peacesoftware.de/einigewerte/wasser_dampf_e.html.

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Appendix.

Appendix question 4

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