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ACTIVE BRAKE COOLING 67 Appendix H: Liquid Distribution System Objective Electronically control spray of a liquid Analysis Positive displacement or non-positive displacement pump? 1. Flow and pressure relationship of a (non-positive displacement) pump When the flow increases, the discharge pressure of the pump decreases, and when the flow decreases the discharge pressure increases (ref. tutorial2.htm). Flow rate would be unsteady in our application 2. Do not let a (non-positive displacement) pump run at zero flow Do not let a centrifugal (non-positive displacement) pump operate for long periods of time at zero flow. In residential systems, the pressure switch shuts the pump down when the pressure is high which means there is low or no flow (http://www.pumpfundamentals.com/centrifugal-pump-tips.htm) The period of running, waiting for pressure relief valve to open would be difficult for a non-positive displacement pump. A Therefore, we should use positive displacement pump type. Flow Control Positive displacement pumps do not slip: If they are turning, they are moving fluid. Rate of fluid delivery to nozzle must be within range of flow rates the nozzle is capable of delivering. With positive-displacement pumps, flow rate is proportional to pump rpm, allowing control of flow rate through control of pump rpm. Requires PWM or voltage control...possible with the Arduino but would require different electronic hardware than we’re been expecting and programming--not our specialty. A mechanical control method is simple:

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Page 1: 1. Flow and pressure relationship of a (non-positive ...€¦ · 2. Do not let a (non-positive displacement) pump run at zero flow Do not let a centrifugal (non-positive displacement)

ACTIVE BRAKE COOLING 67

Appendix H: Liquid Distribution System

Objective

Electronically control spray of a liquid

Analysis

Positive displacement or non-positive displacement pump?

1. Flow and pressure relationship of a (non-positive displacement) pump

When the flow increases, the discharge pressure of the pump decreases, and when the flow

decreases the discharge pressure increases (ref. tutorial2.htm).

Flow rate would be unsteady in our application

2. Do not let a (non-positive displacement) pump run at zero flow

Do not let a centrifugal (non-positive displacement) pump operate for long periods of time

at zero flow. In residential systems, the pressure switch shuts the pump down when the

pressure is high which means there is low or no flow

(http://www.pumpfundamentals.com/centrifugal-pump-tips.htm)

The period of running, waiting for pressure relief valve to open would be difficult for a non-positive

displacement pump. A

Therefore, we should use positive displacement pump type.

Flow Control

Positive displacement pumps do not slip: If they are turning, they are moving fluid.

Rate of fluid delivery to nozzle must be within range of flow rates the nozzle is capable of

delivering.

With positive-displacement pumps, flow rate is proportional to pump rpm, allowing control of flow

rate through control of pump rpm. Requires PWM or voltage control...possible with the Arduino but

would require different electronic hardware than we’re been expecting and programming--not our

specialty.

A mechanical control method is simple:

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ACTIVE BRAKE COOLING 68

…method varies the net forward flow of the pump via an external recycle loop. This most

closely resembles flow control of a centrifugal pump. The recycle valve opens to allow flow

to return to the pump suction. Downstream pressure defines the available pressure drop for

the control valve. The recycle rate will change based on the pump differential pressure and

the control valve opening. This method works best for systems with a high pressure rise and

a constant downstream pressure, e.g., pumping from makeup tanks into a high-pressure

process system.

The recycle system works well with screw, gear and progressive cavity pumps. It is

acceptable for most vane pumps. However, don’t use the method for cyclic pumps such as

reciprocating or diaphragm ones; rapidly changing outlet velocities easily can cause

problems with cyclic pump inlet-head requirements.

(http://www.chemicalprocessing.com/articles/2015/effectively-control-pd-pumps/)

System Schematic

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ACTIVE BRAKE COOLING 69

When electric pump is powered, fluid is moved from the reservoir to the nozzle at a controlled flow

rate. When the pressure at the nozzle reaches a pre-set magnitude, the nozzle sprays liquid.

Required Materials

Description Part # Sold By Price ($) Qty.

Liquid Reservoir 603-001 Amazon 11.74 1 11.74

Tube 6519T13 McMaster-Carr 3.30/ft 10 ft. 33

Tube Clamps 5435K11 McMaster-Carr 5.02 25 (1 pkg.) 5.02

Adjustable spray angle high pressure spray nozzle 3480K21 McMaster-Carr 35.2 1 35.2

In-Line Pressure Relief Valve (brass) RVi-05 Straval 67.15 1 67.15

Brass close nipple 4568K131 McMaster-Carr 1.66 4 6.64

Adjustable sprayer heads - 3.75 5 (1 pkg.) 3.75

Precision Flow-Adjustment Valve for Chemicals 4981K11 McMaster-Carr 58.97 1 58.97

Hose Tee with Barbed Ends 91355K47 McMaster-Carr 6.34 2 (1pkg.) 6.34

Hose Barb Female 1/4 NPT-1/4 Hose Barb 5346K42 McMaster-Carr 14.43 10 (1 pkg.) 14.43

Liquid Pump G2-H 12V 2.5L US Solar Pumps 46.38 1 46.38

Total 288.62

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ACTIVE BRAKE COOLING 70

Plus Tax: 331.913

Description Link

Liquid Reservoir https://www.amazon.ca/Dorman-603-001-Coolant-

ReservoirBottle/dp/B000E35UV2

Tube https://www.mcmaster.com/#standard-plastic-and-

rubbertubing/=1544w7w

Tube Clamps https://www.mcmaster.com/#standard-plastic-and-

rubbertubing/=1544w7w

Adjustable spray angle high pressure spray nozzle https://www.mcmaster.com/#spray-tips/=156irs6

In-Line Pressure Relief Valve (brass) http://straval.com/products/relief-valves/rvi-05/?size=19#size_table

Brass close nipple https://www.mcmaster.com/#brass-close-nipples/=157jtsi

Adjustable sprayer heads

https://www.amazon.ca/Adjustable-Sprayer-Misting-Watering- Irrigation/dp/B014FCRUT2/ref=s9_simh_gw_g86_i1_r?pf_rd_m=A3DW

YIK6Y9EEQB&pf_rd_s=&pf_rd_r=5R18V10XZRBE1PG4QRH9&pf_r d_t=36701&pf_rd_p=b420c7ed-0dc7-4f64-

becab1a9f89477f6&pf_rd_i=desktop

Precision Flow-Adjustment Valve for Chemicals https://www.mcmaster.com/#flow-control-needle-valves/=15bs9se

Hose Tee with Barbed Ends https://www.mcmaster.com/#hose-tees/=15bsf2a

Hose Barb Female 1/4 NPT-1/4 Hose Barb https://www.mcmaster.com/#barbed-hose-fittings/=1544pbj

Liquid Pump https://www.ussolarpumps.com/product/g2-h-direct-drive-gear-pump/

Appendix E: Pneumatic Cooling System

Objective

Maximize cooling effectiveness while minimizing air consumption and intricacy of a pneumatic

cooling system.

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ACTIVE BRAKE COOLING 71

Figure 1.Candidate configurations

Configuration A B

Flow Rate Control Manually adjusted control

valve

Alter nozzle size or pump rpm

On/Off Energize solenoid valve Energize/de-energize pump

Table 1. Flow rate and on/off mechanism descriptions

Introduction

Two outputs derived from this design work: the scale model, and design of a full-scale,

practical system. Modeling heat transfer and cooling medium flows analytically aids in

S

Compressed Air

Source

Manual Valve

Solenoid Valve

Flow Nozzle

Centrifugal Pump

Flow Nozzle

Configuration B

Configuration A

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ACTIVE BRAKE COOLING 72

development of both systems. The scale model should represent the practical system to the highest

degree permitted by constraints in order to maximize the relevance of knowledge developed

through design, construction, and operation of the scale system to a full scale system design.

It has been found analytically that convective heat transfer with turbulent flow is

significantly more effective in heat transfer per unit of air than laminar flow. This is illustrated in

Figure 2: note the significant increase in rate of cooling at the expense of very little increase to flow

represented by the sudden y-axis shift of theTurbulent series relative to the Laminar.

Figure 2. Laminar vs Turbulent flow

The analytical model was based on an Example from Heat and Mass Transfer: A Practical

Approach, by Yunus A. Cengel (p.428), attached as Appendix A . The knowledge that flow

velocity has such a significant effect on effectiveness of cooling has initiated further investigation

into flow nozzles, and enforces that any optimized cooling system prioritizes flow velocity.

Electronic control of volume flow of cooling fluid is not considered necessary because the

volume of cooling fluid delivered at the optimum velocity may be altered by an existing

mechanism: duration of cooling medium delivery periods.

y = 0.209x + 13.25

y = 0.586x + 24.02

0

20

40

60

80

100

120

140

0 50 100 150 200

Flow Velocity (m/s)

Laminar

Turbulent

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ACTIVE BRAKE COOLING 73

Configuration A

As drawn, the manual valve is used to control flow rate, and the solenoid valve flow

periods. It would be possible to control both flow rate and flow period electronically using a

different type of solenoid, but this would complicate the control system further and what this would

allow control of, is already controllable by other, simpler means. Namely, the manual valve, also

the duration of periods of airflow.

It is possible that the existing air system of a transport truck can handle the additional load

of this cooling with little to no modification. That is, the compressed air source would be the

existing system of the large truck the cooling system is installed on. This may significantly reduce

system hardware cost, a concern of ours included in the Goals, Objectives, and Constraints

document which is guiding design decisions.

Another advantage of this sytem would be the size of air lines running to each brake would

be smaller than that of configuration B for any volume flow rate of gas, due to the gas being more

compressed. As there would be many of these lines in a practical application which would need to

be custom installed and consume real volume of a trucks undercarriage, smaller diameter lines with

their tighter turn radius and smaller diameter may be preferrable over the energy efficiency of

Configuration B.

Configuration B

Flow is turned on and off by energizing and de-energizing the pump, and flow rate is a

function of pump rpm and back-pressure provided by the flow nozzle, in the case of the nonpositive

displacement, centrifugal pump.

Since end use is a low pressure, high flow application, it is possible to use a blower, instead

of a compressor to drive airflow. The processes of compression and decompression with associated

entropy changes, yields higher energy consumption in delivering a certain flow rate of air than a

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ACTIVE BRAKE COOLING 74

blower. The major advantage of this system is its reduced energy (operating) cost, if . It is not yet

understood whether the energy cost associated with moving the air is significant. In a multi-brake

system, configuration B may still require solenoids to direct the air to only the brakes requiring

cooling.

If it turns out by regulation or capacity that the existing truck air system cannot be used to

supply the brake cooling system with air, configuration B is preferred for the simplicity and

corresponding low cost of blowers relative to compressors.

Conclusions

Depending on results of future analysis and further information gathering regarding

auxillary use of truck air systems, a configuration of an air delivery system will chosen for use in

large scale practical applications, and our system model. It is favorable for the small system to

represent the large scale system, in that this maximizes the relevance of the knowledge developed

from the scale model to full scale applications.

Appendix A

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ACTIVE BRAKE COOLING 75

Appendix J: Full Scale Model

Part I

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ACTIVE BRAKE COOLING 76

Objective

Determine air volume flow required at each brake to maintain safe brake temperature under

worstcase circumstances through development of an analytical heat transfer truck braking system

model.

Assumptions:

• Velocity of vehicle is constant

• 10 brakes per truck, share load exactly

• No heat is conducted from the brake drum to neighboring components

Conditions

• Research indicates one of the most difficult sections of road for transport truck drivers in

Canada is a 9 km length of Highway 20 which contains grades up to 18%.

• British Columbia regulations dictate that the mass of any truck and trailer must not exceed

63 500 kg.

• In summer, outdoor temperatures in British Columbia can easily reach 30ºC.

• Brake temperature is 100ºC at beginning of descent, and heat transfer from the drum takes

place at 300ºC.

• Brake drums operate best at 250º C, and temperature should not exceed 450ºC. (Yukon PDF)

• The truck is equipped with 10 identical drum brakes and no engine brake.

Properties

Air properties at 160ºC, 1atm:

(Cengel, p.926)

Analysis

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ACTIVE BRAKE COOLING 77

Total change in elevation:

Period of time over which this change in elevation occurs:

Total potential energy recovered during this descent:

Recovered over a period of 270s corresponds with a power of:

Divided across 10 brakes:

Assume approaching the decline with a brake temperature of 100ºC, all ten drums of this type:

Figure 1. Brake Drum (http://www.truckcomponentsonline.com/HEAVY-

DUTYDRUMS_c_1101.html)

The initial energy possessed by this drum of cast iron and 48kg is:

9 km

arctan 0 . 18 = 10 . 20 ̊

h

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ACTIVE BRAKE COOLING 78

Now to calculate the rate at which energy is leaving the plate

Convection From Outside of Drum

The velocity at which air moves over the outer surface of the drum is approximated as the linear

velocity of the vehicle, though the drum is truly in complex motion relative to the ground, rotating

as it translates linearly. Any “nozzling” effect of components near the brake drum on fluid velocity

is neglected.

The drum is approximated as a hollow cylinder of two different inside diameters.

Figure 2. Approximated brake drum

The area of the drum from which heat transfer by convection and radiation is significant does not

include the area normally bolted against the truck wheel, and is approximated as a plate:

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ACTIVE BRAKE COOLING 79

Figure 3.Heat transfer plate

The area of heat transfer is:

L is considered the width of this plate (depth of the drum).

313 053>10 000 therefore heat transfer equations for turbulent flow are used

Assume heat transfer from drum to environment is occurring at an average temperature of 300ºC

Radiation

Not affected by change in fluid velocity, so calculated as occurring from both the inside and outside

of the drum. For cast iron, Emissivity

In the case of conventional braking systems which are passively cooled, the total rate of heat

transfer from the brake drum to the environment is equal to:

Figure 4.Conventional brake heat transfer

Yielding an increase of temperature of the brake drum to --------- under the stated conditions,

which exceeds safe operating limit of 450ºC (Yukon PDF). This increase in temperature occurs

because . The rate of heat loss can be made to equal or exceed the rate of heat

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ACTIVE BRAKE COOLING 80

generation by the addition of forced convection through the inside of the brake drum. To maintain

a brake temperature of 300ºC throughout the decline, .

In the conventional case;

With the addition of convection to the inside of the drum;

Figure 4. Brake heat transfer with forced convection

Convection From Inside of Drum

3.

Consolidating and algebraically manipulating Eq. 1 through 4, a formula is made which will

indicate flow velocity required to remove energy from the drum at any specific rate.

𝑄 𝑜𝑢𝑡 , 𝑡𝑜𝑡𝑎𝑙 = 𝑄 𝑖𝑛 = 𝑄 𝑐𝑜𝑛𝑣 , 𝑜𝑢𝑡𝑠𝑖𝑑𝑒 + 𝑄 𝑟𝑎𝑑 + 𝑄 𝑐𝑜𝑛𝑣 , 𝑖𝑛𝑠𝑖𝑑𝑒

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ACTIVE BRAKE COOLING 78

Conclusion

At an internal drum airflow velocity of 51 988.7 m/s, the rate of energy leaving the plate matches

the rate of energy added to the plate.

This sample calculation may be used to develop an Excel sheet which can be used to experiment

with system parameters.

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ACTIVE BRAKE COOLING 82

Part II

Objective

Determine the volume flow and corresponding power required to deliver 51 988.7 m/s air to the

drum

Assumptions

• The flow area of the drum is reduced by 30% by mechanical components of the brake

Air behaves as an ideal gas

• The energies required to overcome pipe friction, for elevation changes, and of the kinetic

energy of the gas are negligible

Given

Analysis

Reducing flow area by 30% and calculating Volume flow:

Figure 5. Cooling medium flow area

Using the ideal gas law to estimate the effect of increasing pressure on volume flow required:

T, R, m are assumed constant.

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ACTIVE BRAKE COOLING 83

The power required to compress and supply adequate volume flow of air is

Converting to a more familiar unit of power

Multiplying by 10 brakes

Conclusion

The power required to supply enough air to maintain constant brake temperature through forced

convection under conditions listed above is approximately 1.6 million horsepower.

Increasing the delivery pressure significantly reduces the required volume flow, but does not affect

required supply power, in this model.

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ACTIVE BRAKE COOLING 84

Appendix K: Custom Stand

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ACTIVE BRAKE COOLING 85

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ACTIVE BRAKE COOLING 86

Appendix L: Model Specifications

Brake drums are commonly made from Grey Cast Iron Ht250, g3000. Mechanical properties are

listed below. Performance indicators of the Model are also listed. Please note that these values were

obtained ignoring the systems energy losses such as surface roughness/friction

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ACTIVE BRAKE COOLING 87

Mechanical

property Value Units

Elastic modulus 150 Gpa

Density 7100

kg/m^

3

Possion ratio 0.26 -

Thermal

conductivity 53 W/m K

Specific heat 0.46 kJ/kgK

Weight 43 kg

Parameter Calculated

Quantity

Units Detail

Volume Flow Rate 20.8 CFM 166/8outlets

Volume Flow Rate of

Blower

166 CFM Given

Speed of Impeller 2660 RPM Given

Amps 4.1 Amps Given

Volts 12 Volts Given

Wire Gauge 22 gauge Arbitrary Length is less than

10 feet does not

pose threat

Power 49.2 W P=V*I

Power 0.065 hp conversion

factor(1kW=1.34hp)

Velocity 1056.42 ft/min Volume Flow Rate /

Area

Mass Flow Rate 0.0533 Slug/min Volume Flow Rate

*Density of Air

Mach Number 0.015650667 <3 V/C

Density of air 2.571 *10^-3 Slug/ft^3 Room temperature

Outlet diameter 1.9 inch inch Measured in

Machine Shop

Max Voltage Drop 0.36 - 0.3*12

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ACTIVE BRAKE COOLING 88

Outlet Area 0.019689 ft^2 ((3.14)* outlet

diameter ^2)/4