Report 7 Two flasks

19
Report 7 Two flasks Team Taiwan Franklin Liou

description

Report 7 Two flasks. Team Taiwan Franklin Liou. Problem # 7. H. H. h. ?. ?. Investigate and describe in which tube the water goes up faster and in which the final height is greater. How does this effect depend on the time of heating?. Overview. Introduction Experiment - PowerPoint PPT Presentation

Transcript of Report 7 Two flasks

Page 1: Report  7 Two flasks

Report 7Two flasks

Team Taiwan

Franklin Liou

Page 2: Report  7 Two flasks

2

Problem # 7

H H

h? ?

Investigate and describe in which tube the water goes up faster and in which the final height is greater. How does this effect depend on the time of heating?

Page 3: Report  7 Two flasks

3

Overview• Introduction• Experiment– Experimental Setup– Experiment

• Results and Discussion• Conclusions & Summary

Page 4: Report  7 Two flasks

4

Experiment Setup

•1300ml flask (200ml water)•Hot plate•Oil bath (for heating dry flask)

The heating apparatus and sensors•Pressure sensor•Thermocouple

Page 5: Report  7 Two flasks

5

Experiment Setup

Transparent tube and long ruler

Water reservoir

Page 6: Report  7 Two flasks

6

Experiment

• Initial conditions: 100 oC• Conditions– Flask with and without water– Heating time after reaching 100 oC

(1min, 2min, 5min)• Data– Temperature-Time curve– Pressure-Time curve– Water height-Time curve

Page 7: Report  7 Two flasks

7

Experiment Results: Dry Flask

• Height-Time curve is roughly a saturation curve

• Maximum height: 1.72m

0 200 400 600 800 1000 1200 1400 1600 18000

20406080

100120140160180200

dry, 2min dry, 5min

heigh

t (m

)

time (s)

•Temperature-Time curve is roughly an exponential decay•Max: 103oC, Min:31oC•Decay rate:0.0026

0 300 600 900 1200 1500

40

60

80

100 Dry, 2min Dry, 5min exp fit

Tem

pera

ure

(o C)

Time (s)

Dry Flask after heated at 100 oC for 2 minutes

Page 8: Report  7 Two flasks

Experiment Results: Dry Flask

• Pressure-Time curve is roughly an exponential decay• Maximum pressure: 103 kPa• Minimum pressure: 84 kPa

8

19P kPa

Page 9: Report  7 Two flasks

9

Experiment Results: Wet Flask

0 500 1000 1500 2000 2500 3000 3500 400030

40

50

60

70

80

90

100

wet, 1min wet, 2min wet, 5min

Tem

pera

ture

(o C)time (s)

0 500 1000 1500 2000 2500 3000 35000

2

4

6

8

10

wet, 1min wet, 2min wet,5min

heigh

t (m

)

time (s)

• Height-Time curve is roughly a saturation curve

• Maximum height: 8.6m

•Temperature-Time curve is roughly an exponential decay•Max: 100oC, Min:31oC•Decay rate:0.0011

Page 10: Report  7 Two flasks

10

Experiment Results: Wet Flask

• Pressure-Time curve is roughly an exponential decay

• Maximum pressure: 101 kPa• Minimum pressure: ~ 5 kPa

96P kPa

Page 11: Report  7 Two flasks

11

Results and Discussion

dT T Hdt

tR H RT t T T T e

31.5 304.5oRT C K

71.5H RT T K We can obtain the decay rate , and hence the approximate T(t) function

0 300 600 900 1200 1500

40

60

80

100 Dry, 2min Dry, 5min exp fit

Tem

pera

ure

(o C)

Time (s)

Dry Flask after heated at 100 oC for 2 minutes

•Newton’s Law of Cooling:

Square of residual: 0.99974

Page 12: Report  7 Two flasks

12

Dry flask• Ideal gas law: expansion of dry air~1900Pa

PV nRT 0 0 1V hA P h g n RT

•V0: initial volume•P0:initial pressure•N1: initial mole of gas

h h

•A cross section of tube•R: Ideal gas constant•T: temperature at a given time

0( ) th t h B C De

tR H RT t T T T e

Page 13: Report  7 Two flasks

13

Dry Flask Results

0 300 600 900 1200 1500

0.5

1.0

1.5

2.0

2.5

Heated for 5 min

Hei

ght (

m)

Time (s)

Heated for 2 min

Ideal Gas Assumption

H=64.86-5.00*Sqrt(159.67+7.36*Exp(-0.0312t))

0( ) th t h B C De

Page 14: Report  7 Two flasks

14

Wet flask

5132exp 20.386 ot

R H R

P h gT T T e

•Antoine equation:

•Assuming water vapor replaces all air

0( ) expexp( / )Dh t h B C

E F t G

•Water vapor can fill almost all volume -> condense -> large pressure difference~101300Pa

5132exp 20.386P kT

133.3 , ( , )k Pa T in K P in Pa

Page 15: Report  7 Two flasks

15

Wet Flask Results

0 500 1000 1500 2000 2500 3000 35000

2

4

6

8

10

wet, 1min wet, 2min wet,5min

heigh

t (m

)

time (s)

0( ) expexp( / )Dh t h B C

E F t G

Page 16: Report  7 Two flasks

16

Comparison of Wet and Dry Flask

0 500 1000 1500 2000 2500 3000 3500

0

2

4

6

8

10

wet, 1min wet, 2min wet, 5min dry, 2min dry, 5min

heigh

t (m

)

time (s)

Page 17: Report  7 Two flasks

17

Results and Discussion

Time span of boiling at100oC/ maximum height

1min 2min 5min

Dry Flask 1.72m 1.69mTheoretical Dry Flask (Ideal gas law)

2.25m 2.25m

Wet Flask 8.65m 8.66m 8.42mTheoretical Wet Flask (Antoine equation)

9.12m 9.12m 9.12m

Page 18: Report  7 Two flasks

18

Conclusions & Summary• Two flaks : two mechanisms–Dry flask: expansion of air~ 1.9 kPa–Wet flask: condensation of vapor~ 101300 Pa

• Water rises faster in wet flask condition• Maximum water height is greater in wet flask

0 500 1000 1500 2000 2500 3000 3500

0

2

4

6

8

10

wet, 1min wet, 2min wet, 5min dry, 2min dry, 5min

heigh

t (m

)

time (s)

• Maximum water height and water rising speed is independent of time of heating

Page 19: Report  7 Two flasks

19

0 300 600 900 1200 1500

0.5

1.0

1.5

2.0

2.5

Heated for 5 min

H

eigh

t (m

)

Time (s)

Heated for 2 min

Ideal Gas Assumption