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AIRBUS FLY YOUR IDEAS 2013 TEAM AMAZONS LALITYA DHAVALA M. ANUSYA SOWMIYA MADHIAZHAGAN REVATHY PRIYA R. SIVARANJANI GANAPATHY SANTHANAM DEPARTMENT OF AEROSPACE ENGINEERING AMRITA VISHWA VIDYAPEETHAM ECO-FRIENDLY, ENERGY EFFICIENT CABIN INTERIORS FOR HUMIDITY CONTROL Abstract: The possibility of using humidity buffering properties of clay for increasing the humidity levels in the aircraft cabin is investigated. By increasing the humidity levels in the cabin, passenger experience is improved thus, resulting in higher number of passengers and more revenue for airlines and aircraft manufacturers alike.

Eco-friendly eco-efficient cabin interiors for humidity control

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AIRBUS FLY YOUR IDEAS 2013

TEAM AMAZONS

LALITYA DHAVALA

M. ANUSYA

SOWMIYA MADHIAZHAGAN

REVATHY PRIYA R.

SIVARANJANI GANAPATHY SANTHANAM

DEPARTMENT OF AEROSPACE ENGINEERING

AMRITA VISHWA VIDYAPEETHAM

ECO-FRIENDLY, ENERGY EFFICIENT CABIN INTERIORS FOR HUMIDITY CONTROL

Abstract: The possibility of using humidity buffering properties of clay for increasing the

humidity levels in the aircraft cabin is investigated. By increasing the humidity levels in

the cabin, passenger experience is improved thus, resulting in higher number of

passengers and more revenue for airlines and aircraft manufacturers alike.

1 Objectives : To present initial approximate estimates of the amount of increase in humidity levels

and reduction in pressure differential for the cabin, by replacing cabin interiors with

clay and other natural materials.

• To propose methods of incorporating clay into the cabin, and limitations and

requirements for the same.

1.1 Approach: It was decided that a thorough understanding of how and why an aircraft cabin is maintained

at low humidity levels was to be the first step. We then, planned on proceeding to studying the

properties of clay and its present use world-wide. With the ideas clear, we concluded that an

analytical study to characterize the capabilities of clay and an experiment to demonstrate the

mechanism would be the best way to justify our proposal.

2 Description 2.1 Research/Background Information of Current Cabin Conditions This section presents results of background research into current cabin environments and clay

properties etc.

2.1.1 Survey: As a first step towards identifying the problems faced by passengers in airplanes, we conducted

a survey of around 30 people who were frequent flyers asking them to identify and rate the

factors which they felt was the most inconvenient during air travel. The economy class was

targeted as that is where the passengers face the most discomfort with airlines and aircraft

manufacturers dishing out various luxuries for the higher- end classes. The questionnaire used

and a sample response is attached as Appendix I.

Figure 1: Problems faced by customers in aircraft cabins.

As we can see from the graph above, problems of low humidity maintained in the cabin were

felt by almost one- third of the passengers surveyed. This is why we decided that we shall focus

on trying to find a solution for this problem.

2.1.2 Study of Environmental Control System: We made a thorough study of the ECS used in aircraft cabins. The present humidity level

maintained by the ECS is around 10-15 % [7] and currently, human perspiration is the only

source of humidity in the cabin.

2.2 Study of the Properties of Clay : This section presents result of research into clay properties.

2.2.1 Clay Behavior / Humidity buffering by clay: When clay is exposed to a high humid environment (higher than the average room humidity), it

adsorbs moisture. This adsorbed moisture content ( in terms of amount of water vapour ) is

released when it is exposed to low humid environment. .

Water is adsorbed onto the surface of the clay when the moisture content in the clay is less

than the ambient relative humidity. The water penetrates only up to a certain depth known as

the penetration depth, where the moisture content in the clay will reach a point of equilibrium

with the ambient conditions. The thickness of the adsorbed water layer is a point of debate

among researchers, where it is argued that the water is adsorbed as a mono layer or up to ten

layers depending on the type of clay and amount of water concentration in the clay.

Figure 2 : Clay texture

Adsorption and desorption phenomena in clay are controlled by the differential entropy of the

water molecules in the clay and in the surrounding atmosphere. The nature of this adsorbed

water has been found to have an effect on the mechanical, thermodynamic, magnetic and

dielectrical properties of the clay. Clay also shows a swelling behavior when it adsorbs water

since it is an expansive soil but it has been proved that there are no potential problems due to

this behavior pertaining to its use in construction [2]. Studies have been performed on the

relation between swelling pressure experienced by the clay molecules and its moisture content

(G.Kahr et.al, Clay minerals 1990).

The ability of clay to absorb water vapour during periods of high humidity and release it during

periods of low humidity is knows as humidity buffering. This property helps to maintain a

constant relative humidity in the cabin. The amount of buffering increases as the amount of

clay used increases.

The amount of buffering or the damping of the RH cycle depends on four factors:

• Material’s capacity for absorbing water vapour

• Water vapour permeability

• Interaction of absorption and permeability in a dynamic situation

• The effect of ventilation

2.2.1.1 A Material’s capacity for absorbing water vapour: The adsorption and desorption of water vapour by clay is represented in a sorption

isotherm, which is a graph of how much water vapour is adsorbed or released by a type of clay

at a specified partial pressure.

There are several models according to which adsorption isotherms can be constructed such as

Braueneur-Emmett-Teller theory and Dubinin-Serpinski equation. The D-S equations result in

a simple isotherm model as follows: [10]

Where q= amount of water adsorbed or adsorption capacity at a specified partial pressure

Q0=limiting adsorption capacity at relative pressure approaching 1.0

K= proportionality constant

P=actual partial pressure of water vapour

Po= saturation partial pressure of water vapour

The limiting adsorption capacity is related to the limiting pore volume by the relation[10]

Where Vo= limiting pore volume

Ρ= density of condensed adsorbate i.e. water vapour in this case

The extent of adsorption depends on the cations present in the type of soil as well because the

primary reason of adsorption is the electrostatic attraction between the dipolar water molecular

and the cations present on the surface of the clay. The effect of different cations on the

adsorption properties of clay had been investigated[2].

Figure 3 : Clay soil Mechanics

2.2.1.2 Water vapour permeability:

Water vapour permeability is defined as the weight of water vapour transmitted through a

meter cube of material with a pressure difference of 1 Pa across it. This has been

experimentally characterized for various bricks made of different types of clay. From this study,

the value of water vapour permeability for a smectite brick was noted as 8.55e-12 kg/m.s.Pa [19].

2.2.2 Interaction of absorption and permeability in a dynamic situation: The humidity buffering property of the clay is due to two distinct phenomena:

adsorption/desorption and diffusion. Presently, there is no theory that describes the

combination and inter-dependence of these factors (how one affects the other).

The diffusion through materials is generally assumed to follow Fick’s law of diffusion which

states that the rate of diffusion through a porous material is proportional to the water potential

gradient. Though there are some computer programs[17] which calculate the amount of

diffusion in rooms built with porous materials, they take wall relative humidity as a boundary

condition, which is not the case when applied to humidity buffering concept.

Also there are two factors which can drive the humidity buffering property: vapour pressure

gradient and relative humidity gradient. Though both are similar concepts, the identification of

the correct driving potential makes a change in the estimates of humidity buffering and there is

no analytical procedure yet to distinguish between the two in the case of clay.

The theoretical performance of clay as a humidity buffer can be characterized in terms of:

• Moisture effusivity

• Moisture Buffer Value

2.2.2.1 Moisture effusivity:

The capacity of a material to buffer humidity can be defined with an analogy with the thermal

effusivity property in heat transfer studies. This is a material property defined at a constant

water vapour saturation pressure. The water vapour saturation pressure depends on the test

conditions.

For a test condition temperature of 220C , the ability of clay to absorb or release moisture can

be calculated as

Where δp= water vapour permeability=8.55*10-12

Ρo= dry density of the material=593 kg/m3

(See Appendix III)

Ps=saturation pressure at 220C=2.639 kPa

2.2.2.2 Moisture Buffer Value

The second parameter to characterize the moisture buffering properties of clay is termed as the

Ideal Moisture Buffer Value. It is defined as the moisture uptake/ release of a material

normalized to the change in surface relative humidity. Practically, Moisture Buffer Value,

MBVpractical, is the change of mass of the material per square meter of surface area per change

in Relative Humidity. [11]

This value of Moisture Buffer Value is under the ideal case where the following assumptions

are used:

• The surface resistance of clay towards sorption and diffusion is considered to be

negligible.

• The sample is in steady state and initially in equilibrium with surrounding atmosphere.

• The thickness of the material used is higher than its penetration depth.

• The variation of ambient moisture follows a sinusoidal variation in time with the period

of high humidity lasting for one-third of the time that period of low humidity exists.

• The effect of ventilation is not considered.

2.3 Theoretical Calculations This section presents analytical calculation of relative humidity vs mass of clay, using the

sorption isotherms and the theory discussed above.

Typically, for Cabin Width, w = 3.68 m

and Cabin Length = 27.51 m

Instead of covering the full cabin length, we can divide it into ten sections, and use clay coating

in one of the sections. So, the effective length of the clay coating, l, is 2.751 m.

Surface Area of the clay coating on the cabin wall = 2πrh

Where, r = = 3.68/2 = 1.8400 m

h = l = 2.7510 m

Surface Area =

= 31.8045 m2

Volume, V =

=

= 0.6361 m3 = 636089.58 cm3

Considering that the cabin from the floor to the ceiling is a semi-circle,

Total volume of the clay coating, =

=

= 318044.79 cm3

Density of the clay, ρ = 2.35 g/cm3

Mass of clay required =

= 2.35 318044.79 = 1494810.513 g

= 1494.8105 kg

Assuming that,

The present aircraft interior cabins are at a relative humidity of 10%,

The clay, Montmorillonite, releases 0.5 mg water vapour per 1 gm of clay at the cabin

condition. (from sorption isotherms, Appendix II)

This implies, 1494.8105 kg of clay will release 0.7474 kg water vapour.

This water vapour fills the cabin of volume 139 m3.

That is, there is, 0.005377 kg/m3 water vapour in the cabin.

This can be expressed as[8]

Where, Pa is the actual pressure of the water vapour

T is the temperature inside the cabin, assumed to be 22oC

This implies,

0.005377 = (0.002166 Pa) 295.16

From the above, we get,

Pa = 734.7569 Pa = 0.7348 kPa

RH = [(actual pressure of water vapour) (saturation water vapour pressure)] 100

Saturation water vapour pressure at 22oC is 2639 Pa

Hence,

RH = (734.7569 2639) 100

= 27.8%

Table 1 : Requirements of clay and increase in cabin pressure for specific increases in RH

Net increase in RH (%)

Mass of the Clay (Kg)

Surface Area (m2) Increase in Cabin Pressure (decrease in pressure

differential) (kPa) 27.8 1494.8105 31.8045 0.7348 30 1613.1049 34.3214 0.7929 35 1881.9557 40.0416 0.9250 40 2150.8065 45.7618 1.0572

The Theories discussed above and the corresponding calculations were purely based on only

adsorption and desorption. Diffusion hasn’t been accounted for in the above calculation.

Experimental results might give a closer value to reality.

2.3.1 Reasons behind choosing montmorillonite for characterization of practical Moisture

Buffer Value: • The extent of water adsorption varies with the type of clay and montmorillonite clay has

a very high surface area[12]. Clay soils are very compact and cohesive giving them ability

to store water in its pores.

• A comparison of the adsorption isotherms of samples of montmorillonite, kaolinite and

illite clays show that montmorillonite has the highest water adsorption and desorption

capacity but its hysteresis is also large. (Refer Appendix II). These sorption isotherms

are generally reproducible and can be interpreted with the help of Brunauer-Emmett-

Teller theory on the adsorption of gases onto a solid surface.

Figure 4 : Illite Figure 5: Kaolinite

Figure 6: Montmorillonite

• From experimental studies. It has been found that montmorillonite clay with perlite

filler is the best material for humidity buffering[12].

Figure 7: Perlite

2.4 Experiment to Characterize the Practical Moisture Buffer Value

2.4.1 Aim : To demonstrate the principle of moisture buffering property of clay and to obtain the practical

moisture buffer value of the clay for our sample. This will be done by plotting the variation of

mass of the clay as a function of days.

2.4.2 Principle : The change in the moisture content of the clay can be characterized as the increase in weight

of the sample during moisture adsorption cycle and decrease in the weight during moisture

release cycle.

In the context of our experiment, the practical Moisture Buffer Value is obtained as the

moisture uptake or release in the test environment simulated. This Moisture Buffer Value can

be quantified by monitoring the change in the weight of the sample over the 8 hours/ 16 hours

cycles. It is normalised over 1 square meter of surface area for a unit change in Relative

Humidity.

2.4.3 Test Environment maintained during the experiment: The system is kept at the room temperature of 30oC. The sample is exposed to high Relative

Humidity of about 92% for 8 hours continuously and then exposed to low Relative Humidity of

about 51% for 16 hours. This cycle is repeated for a period of three days. These Relative

Humidity values are maintained using saturated salt solutions as saturated salt solutions are

known to supply water vapour to maintain a specific RH in its immediate surroundings.

2.4.4 Test Apparatus : • A box that provides moisture insulation, in other terms, air tight.

• Saturated Salts (Sodium Chloride, Magnesium Chloride, Potassium Chloride, Potassium

Nitrate, Magnesium Nitrate)

• A Sample of Montmorillonite Clay

• Analytical Balance

• Whirling Psychrometer

2.4.5 Setting Up the test system: • The Climatic box (that provides moisture insulation) is initially filled with saturated salt

solution of the salt that maintains high humidity. This is basically a very wet form of

salt. This is filled up to about 3mm in height of the box.

• The sample of the montmorillonite clay (Fuller’s Earth) is taken in its dry / raw form in

a plastic box of surface diameter of its open end about 11.2cm.

• The plastic box is to ensure that the clay adsorbs only through its exposed surface area

of 98.5203cm2

• This sample is first weighed for an initial reading.

• It is then, placed inside the box containing the saturated salt solution and the box is

tightly closed and kept.

• After 8 hours, the sample is taken out of the environment and weighed and the value is

noted.

• The Saturated salt inside the box is replaced now with saturated solution of the salt

that maintains low relative humidity, filled up to about 3mm of the height of the box.

• The sample is then placed inside and left.

• After 16 hours, the sample is again taken out and weighed and the value is noted.

• This cycle is repeated for a period of 3 days.

This experimentation is followed by the calculations as below.

Figure8a Figure8b

Figure 8 a,b,c : Clay sample and the experimental setup

Figure8c

Figure 9 : Weighing the sample

2.4.6 Experiment Trials:

2.4.6.1 Trial 1 :

For our first trial, we used a slightly wet clay, with the combination of Sodium Chloride (NaCl)

and Magnesium Chloride (MgCl2.6H2O) for simulating the desired Relative Humidity difference

inside our test chamber.

2.4.6.1.1.1 Error

From the start, there hasn’t been any observable change in the clay mass and we couldn’t

proceed forward with the same.

2.4.6.2 Trial 2 :

We took a completely dry sample of clay this time, for the same combination of salts.

NaCl maintains 75.09% RH

MgCl2.6H2O maintains 32.44% RH

We expect the mass increase in the presence of NaCl and decrease in the presence of

MgCl2.6H2O

This time, we checked for the mass change every one hour.

Initially we have kept NaCl for moisture adsorption.

2.4.6.2.1.1 Observation :

S.No Duration

(hours)

Mass of the

sample (g)

Change in

mass (g)

1. 0 115.315

2. 1 115.487 0.712

3. 2 115.683 0.196

4. 3 115.69 0.007

5. 4 115.853 0.163

6. 5 115.806 -0.047

7. 8 115.905 0.099

SALT CHANGE TO MgCl2.6H2O

8. 0 115.905

9. 1 116.014 0.109

10. 2 115.915 -0.099

11. 10 116.47 0.555

12. 12 116.869 0.399

13. 13 116.892 0.023

2.4.6.2.1.2 Error

From the observation, we could see that there is an erratic behaviour in the moisture adorption

and release of the sample.

This might be due to :

Improper salt content or composition

or

Disturbing the isolated system in between so many times.

So, we went for our third trial.

2.4.6.3 Trial 3:

We used the same sample as in trial 2, but with the combination of Potassium Chloride (KCl)

and Magnesium Nitrate (Mg(NO3)2.6H2O) for simulating the desired Relative Humidity difference

inside our test chamber.

KCl maintains 83.62% RH

Mg(NO3)2.6H2O maintains 51.4% RH

We expect the mass increase in the presence of KCl and decrease in the presence of

Mg(NO3)2.6H2O

We left the sample in the test chamber for 8 hours and 16 hours respectively, without

disturbing it.

2.4.6.3.1.1 Observations:

S.No Duration

(hours)

Mass of the

sample (g)

Change in

mass (g)

1. 0 112.21

2. 8 113.23 1.02

SALT CHANGE TO Mg(NO3)2.6H2O

3. 0 113.23

4. 16 114.645 1.415

SALT CHANGE TO KCl

5. 0 114.645

6. 8 117.771 3.126

SALT CHANGE TO Mg(NO3)2.6H2O

7. 0 117.771

8. 16 117.859 0.088

2.4.6.3.1.2 Error

We observed that, the behaviour in the presence of these salts is not as expected.

This might be due to:

Improper salt content or composition

Or

Insufficient RH difference between the high and the low RH cycles.

So, we started our fourth trial.

2.4.6.4 Trial 4 :

We used the same sample as in trial 2 and 3, but with the combination of Potassium Nitrate

(KNO3) and Magnesium Nitrate (Mg(NO3)2.6H2O) for simulating the desired Relative Humidity

difference inside our test chamber.

KNO3 maintains 91.31% RH

Mg(NO3)2.6H2O maintains 51.4% RH

We expect the mass of the sample to increase in the presence of KNO3and decrease in the

presence of Mg(NO3)2.6H2O

We left the sample in the test chamber for 8 hours and 16 hours respectively, without

disturbing it.

Initially, we started with KNO3.

2.4.6.4.1.1 Observations

S.No Duration (hours)

Mass of the sample (g)

Change in the mass (g)

1. 0 186.52

2. 8 188.852 2.332

SALT CHANGE TO Mg(NO3)2.6H2O

3. 0 188.852

4. 16 187.643 -1.209

SALT CHANGE TO KNO3

5. 0 187.643

6. 8 188.649 1.006

SALT CHANGE TO Mg(NO3)2.6H2O

7. 0 188.649

8. 16 188.052 -0.597

SALT CHANGE TO KNO3

9. 0 188.052

10. 8 188.901 0.849

SALT CHANGE TO Mg(NO3)2.6H2O

11. 0 188.901

12. 16 188.212 -0.689

2.4.6.4.1.2 Calculations

Average change in mass during a cycle: Average of the mass changes in the presence of KNO3

and Mg(NO3)2.6H2O respectively.

First Cycle: Average mass change = (2.332 + 1.209)/2 = 1.7705g

Second Cycle: Average mass change = (1.006 + 0.597)/2 = 0.8015g

Third Cycle: Average mass change = (0.849 + 0.689)/2 = 0.769g

Average mass change over three cycles, m: (1.7705+0.8015+0.769)/3 = 1.1137g

= High humidity – Low Humidity = 91.31 – 51.4 = 39.91

Surface Area, A = = = 98.5203 cm2

Moisture Buffer Value, MBVpractical = = = 0.28mg/cm2 per unit change RH.

From, section 2.3 (theoretical calculations), 27.8% RH corresponds to 0.7474kg water vapour

transport.

From the above Moisture Buffer Value, 0.28mg of water vapour is released per cm2 surface

area.

That is, to obtain 0.7474kg water vapour, surface area of clay coating required is 266.9286 m2

which corresponds to 12545.644kg

Figure 10 : Variation of mass of the sample over time

As can be seen from the graph, the slope of the graph changes every cycle. That is, over time,

the rate of moisture uptake and release degrades.

3 Outcomes : Many airlines provide air-humidifiers for their first class customers, while the economy class is

left to face the challenges of less humid environment. The justification is that, the operating

cost increases monumentally for the use of these throughout the aircraft cabin. Through our

work, we propose an alternative that would increase the humidity inside the cabin at much

lower cost. With a proper initial humidification, the material we are proposing (Montmorillonite

clay) will release water vapour, thereby, effectively increasing the humidity inside the cabin.

The proposed system is eco-friendly, and energy efficient. It is also bio-degradable, meaning,

disposal after use is made easy and environment friendly. Also, there is an increase in the

cabin pressure, which consequently increases passenger comfort.

We have predicted, by theoretical analysis, that there is an overall increase of 27.8% in the

relative humidity of the cabin and an increase of 0.7348kPa in the cabin pressure, with the

use of 1494.8105Kg of clay spread over an area of 31.8045m2 with the thickness of 0.02m

(20mm). The increase in the pressure is the reduction in pressure differential required.

Through our experiment, where we have used the Fuller’s Earth form of Montmorillomite clay,

to obtain an overall increase of 27.8% RH in the cabin and an increase of 0.7348kPa in the

cabin pressure, 12545.644kg of clay spread over 266.9286m2 has to be used.

By increasing the humidity levels in the cabin, passenger experience is improved thus,

resulting in higher number of passengers and more revenue for airlines and aircraft

manufacturers alike. The increase in weight and the consequent increase in fuel consumption,

can be offset by the use of bio-fuels, and more lighter composite structures (natural fibers have

very less density) for the aircraft.

4 Recommendations 4.1.1 Integration into Cabin The quantification we have done is for pure montmorilomite clay material. We propose that a

coating of a thin film of clay of thickness about 20mm is added in the interior surface of the

cabin wall. Clay can also replace the present day class dividers, carpet area, Seat backs,

overhead boards and wherever a continuous surface area can be found. Clay has micro-

hardness and its strength is not appreciable. So, to be used as these replacements, the

strength of clay has to be improved. The mechanical properties of clay increase with the

use of natural fibres and straw as reinforcements. One such natural fiber that we propose

is Vetiver grass.

Figure 11 : Clay Coating inside the cabin

Vetiver grass is moisture absorbent. So, when used as reinforcement for clay, a proper

moisture absorption study has to be done for it, and accordingly amount of clay required for

the effective increase in relative humidity has to be calculated.

From the researches, it is understood that the buffering property of clay is purely a

surface property and thus, they can’t be used in the form of clay reinforced polymer

composites, where, clay is generally a nano-filler.

4.1.2 Initial Humidification For Moisture Buffering to work, initially there has to be humidification prior to flight. We

propose that, since cabin RH is about 10% , the cabin has to be humidified to a 50-60% RH at

the least. CTT systems’ humidifiers are presently in use in A380 for crew comfort. These

systems can be used to humidify the cabin before flight, for about half the duration of

the total flight. In places where natural RH is high, just a proper ventilation (about as

much as in typical houses) inside the cabin before flight would be sufficient, leading to

an almost zero input humidification system.

4.1.3 Scope For Improvement It has been studied that the effectiveness of moisture buffering increases with the

presence of moisture absorbents in the environment[5]. We propose that many of the

plastics in use inside the cabin could be replaced by natural fibers and substances that

are moisture absorbent.

Our Suggestions for some of these replacements:

Plastic water bottles and juice bottles – Bottle guard bottles

Added benefit: “The large bottle gourds are extremely useful among the

country people, by whom they are used as dippers. They are light, and

with good usage may last for months and even for several years.” - The

Farmer’s and Planter’s Encyclopaedia of Rural Affairs.

“These gourds were much preferable… for water, in these would remain

cool through the day of the hottest sun” – Journal of a private in

Tennessee Regiment of Cavalry in the campaign in Mexico

Soup and Salad Bowls – Clay-pot bowls

Plastic Sachets – Fiber/Bagasse sachets with silica gel packet inside for keeping

the food fresh

Plastic Plates and Spoons, Plastic cups for hot and cold beverages – Areca Palm

Bark plates, cups and spoons

Clay Containers with vetiver grass put in for water storage

Added Benefit: keeps water cool and thus, reduced refrigeration

required.

Our calculations are subject to assumptions aforementioned and the corresponding

changes in the values due to change in the operating conditions have to be taken into

consideration.

All our work has been done for pure clay and only desorption effect has been considered

during analytical quantification. The effectiveness of the humidity buffering can be

increased using Perlite as filler which helps in opening up the pores of the clay and

consequently increases the diffusion effects.

The ideal mixture of montmorilomite and perlite is :

For 1 volume of montmorillonite, 1.5 volumes of water and ten volumes of

perlite.

Fuller’s Earth form was the only form we tested. Other forms of Montmorillonite might

produce better results for very less increase in weight. Those should be tested for the

same and the best should be selected for implementation.

As seen from the experimental results, there is degradation of the buffering property of

clay over time. Thus, the life time of the clay that is going to be used should be

estimated. This can be done by doing the same experiment as we have discussed till

there is no change in the mass. This will effectively give us the time when the buffering

stops.

4.1.4 Limitations Humidity buffering has been found to be effective for ventilation rates of about 1 air change per

hour. In airplanes, typically there is about 1 air change every 2 minutes. Thus, the

effectiveness of the clay has to be tested in a similar environment before implementation.

4.1.5 Feasibility of the idea As mentioned earlier and observed in one of our experiment trials, ventilation could be a major

problem for immediately implementing the idea. The proposal could be efficiently implemented

once the moisture buffering of clay is properly characterized for the ventilation conditions of

the cabin during flight.

CHECK-LIST TO COMPARE WHAT WAS PROPSED AND WHAT HAS BEEN ACCOMPLISHED

*Appendix IV for Round 1 Proposal

ACKNOWLEDGEMENTS:

We would like to extend our whole-hearted thanks to Airbus, for providing us this wonderful

opportunity to ‘fly our ideas’. We would like to thank the Chairperson, Department of

Aerospace Engineering, Amrita Vishwa Vidyapeetham and its faculty members for their

encouragement throughout the course of the project. Our sincere thanks to the academic mentor,

Mr.T.Rajesh Senthil Kumar, M.Tech, Assistant Professor, our Airbus mentor, Mr.Boonseng soh and

Airbus expert Mr. Berend Schocke, who provided us with their guidance and invaluable

assistance. We wish to thank the Department of Science, its faculty and lab in-charges for

assisting us with the facilities required. We wish to express our gratitude to our friends for

their help and support.

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