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1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

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Page 1: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

1

Steps in Design of a Hoisting System

©Dr. B. C. Paul 1999 major revision 2012

With Credit to Dr. H. Sevim for Original Book

Page 2: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

2

Steps in Design of Hoisting System Determine the performance requirements

• Usually means production• can also involve figuring acceptable stopping

distances - number of levels to be served under what conditions

Select hoist type to meet constraints

Page 3: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

3

Once Upon a Mine

Dark Black coal mine will produce 3 million tons of coal from a single level. The hoisting distance from loading pocket to dump bin is 1000 ft. The mine operates 250 days per year 3 production shifts per day with 7 hours of operation each production shift. The peak production will be about 5000 tons per shift. The average production is 4000 tons per shift.

Page 4: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

4

Your Mission Jim, Should you decide to accept it Design a hoisting system for the Dark Black Coal

Mine.

First Step is to establish the performance requirement.

The fundamental Capacity Equation is• Q = P / T• Q is requirement in Tons Per Hour• P is Production per shift• T is the average shift production time

Page 5: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

5

Which Production Number Do We Use? Actual production is a distribution - not an

average number If we design on average then all the

numbers above the mean will go past capacity - we’ll loose our high values and not meet production

If we design on a peak that is seldom achieved we’ll pay big bucks

Page 6: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

6

Decision Criteria

If peak approaches 2 times average - need to consider cost of work stoppage vs. take work stoppages

If peak is somewhat close to average then design for the peak

In example the peak is 125% of the average, which is not considered a significant deviation. Design for the Peak!

Page 7: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

7

What if Life had not been so Kind? Calculate the cost of a production stoppage

• May be cost of lost production• May include penalties on contracts• May include idle labor cost

Calculate the amortized cost of the next increment of production capacity

Check multiple points and go for minimum total cost.

Page 8: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

8

Pick production capacity Apply formula

• 714 tph = 5000 t/shift / 7 hours prod time

Other design decisions need to be made• Is this a Keope or a Drum Hoist?• One Level so Keope won’t be too tricky

Page 9: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Input My Hoist Distance and Production Rate Target

9

My Spreadsheet isOpti-Hoist.

Next Lets look at some fixedCycle time elements

Page 10: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Elements

How Long will it take for the ore pocket doors to open and drop a load into the skip?

Once the Skip is in position how long will it take to deposit the load into the dump point chute?• About 8 seconds to load• 10 seconds to dump is reasonable• Your load and unload times may depend on other

design elements of the system.10

Page 11: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Creep Time

Hoists and Elevators slow to near stop as they line up with a set level• Pull away fromthe loading point

• Or line up with dump point

• Will Usually take a bit more time to line up with the unload point

• 2 seconds to pull away from load and 4 to line up with dump is reasonable.

11A fowl Beast

Page 12: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Now We Need to Pick a Peak Speed and a Rate of Skip Acceleration

12

The maximum speed we lift at is safety related. For men there are regulations.For materials there are guidelines (shown in pink)

Page 13: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Considerations

This is a Keope Hoist• The rope is just sitting over a friction wheel• If I “peel out” and the rope starts to slip I have

a major hoisting accident

High speed and high acceleration increase production• But they also cause a big increase in motor size

and energy bill.

13

Page 14: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

I’m going to go for modest speed and particularly modest acceleration

14

Page 15: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Geometry Considerations

15

Two Skips Skip and Counter-weight

Page 16: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Stopping Considerations

16

If my controls missStopping the skip atThe dump point – howFar do I have for anEmergency stop beforeThe over-wiend turnsInto a disaster?

DumpChute

Loading chute

Shaft Bottom

Page 17: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Getting Our First Estimate

17

Using a Nordberg approximation of the cycle time the program estimates the sizeOf skip that will be needed to achieve the production target using the distance,Speed and acceleration conditions specified.(This part of the spreadsheet is independent of whether the hoist was a Keope orA drum hoist).

Page 18: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Our Next Task is to Get Our Exact Cycle Time

18

The only missingPiece of informationWas what is theCreep speed (2 ft/secIs reasonable).

(I want’s you money for my fakeGlobal warming initiative)

Page 19: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Next We Must Balance Skip Size, Weight, Rope Diameters and Wheel Sizes

19

Page 20: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

First We Need to Pick A Skip Size

20

We have already been given a first guess skip size. We try about that sizeAnd then check the actual hourly production achievable in the red box (weNow have figured the exact cycle time too).

As can be seen a 16 ton skip will get me my 720 tons/hour.

Page 21: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Next I’ll Go for Skip Weight

21

In general a skip heavy enough to handle the banging of ore loading andUnloading will weight about 75% of the load weight.

Opti-Hoist estimates this for us but leaves us a yellow blank to choose theWeight. A higher weight usually means we are just adding weights to ourSkip.

Page 22: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Next We Go For Rope Sizing

22

Keope hoists usually have multiple ropes in even numbers, 2, 4, 6, and 8 beingCommon. Where that 12 came from is unsure.

We need to consider both hoisting ropes and tail ropes. Sometimes tail ropesAre used and worn-out hoist ropes which can cause tail ropes to be the sameAs hoist ropes.

Page 23: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

My First Guess is 4 ropes(This is a relatively modest depth)

23

The red box estimates that I will need a 1.064 inch rope to reach neededSafety factors for this depth.

Page 24: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

From Here I Need to Go And Enter My Rope Properties

24

I enter my rope size, it’s weight and it’s strength. (I have the advantage ofHaving an estimate of what size rope to try).

The spreadsheet then compares the achieved factor of safety to what is required

Page 25: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Where Do I Get These Rope Properties

25

The spreadsheet has aRope properties tableRight below for me toLook things up on.

I’m looking for 1.064Flattened strand

I go for 1.125Weight 2.28 lbs/ftStrength 57.9 tons

Page 26: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Enter My Rope and Check My Factor of Safety

26

A 7 factor of safety clearly meets a 6.5

Page 27: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

I Wonder If I Could Get Away with a 1 inch rope

27

Eeee – one inch rope is a nope.

Page 28: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

What if I Use High Strength Steal?

28

Oh so close but still nope to the rope

Page 29: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

With Hoist Rope Selected I can now pick the Wheel for My Hoist Frame

29

I need a 7.5 ft wheel (see pick recommendation) to avoid bending my rope toSharp. (You can see why I wanted a smaller rope – it would have allowed meTo use a smaller lower inertia wheel).

Page 30: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Now I Need to Deal with Tail Rope Simple case is to get used rope Also easiest to have just one tail rope so

have less swinging and tangling. Number of tail ropes is commonly less than

number of hoist ropes.

30

Page 31: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

I’m going to try straight across Using my worn-out hoist ropes for tail ropes.

31

Page 32: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Now I’ll Check Conditions at My Keope Wheel

32

T1 is the weight of the heavy loaded side. T2 is the weight of the lighter emptySide.

Remember – only friction stops the rope from slipping. The ratio of T1 to T2Must therefor not be more than 1.5

Of course 1.95 is greater than 1.5 so life is sucking right now.

Page 33: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Another Parameter is Tread Pressure

33

Keope wheels are normally lined with a leather like frictional material. Since weDon’t want the ropes to cut the material to pieces we need to limit the load toAbout 300 psi or less.

Well at least one thing worked.

Page 34: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

So What Do I Do Now

Either T1 is to big or T2 is too little I could look at rope weight but the rope weight

shifts back and forth from T1 to T2 depending on where we are• The T1 and T2 ratios are picked by the spreadsheet to

be worst case

I could make my skip lighter• But a light duty skip could get beat to pieces• And a lighter skip would also reduce T2

34

Page 35: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Idea

If my skips were heavier then the skips would account for a higher percentage of the weight.

Since skips are the for T1 and T2 making it a larger proportion will even the ratio

(I could make a similar argument for picking heavier ropes but ropes are expensive and big ropes for larger higher inertia wheels).

35

Page 36: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Putting 8 tons of Dead Weight on My skips made it more even

36

Of course I’m still not there yet.

Page 37: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Ok – Adding 15.5 dead weight tons to the skip did it!!!

37Oh boy did it do it – take a look at that tread pressure.

Page 38: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

So What Can I Do With My Tread Pressure I can’t change my T1 and T2 But I can spread the load over a greater area

• That unfortunately would mean getting a bigger Keope wheel

38

Page 39: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

There – A 10 ft Wheel Spreads the Load

39I know – the inertia situation sucks.

Page 40: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Come to Think About It – The Factor of Safety Sucks Too

40

How profound – I put more weight on the rope without strengthening the ropeAnd I get into safety factor trouble.

(Where theMoney Goes)

Page 41: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Take A Little Weight Off the Skip and Put A Little More On the Rope

41

Page 42: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Time to Pick Out Our Motor

42

Page 43: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

43

Looking at Hoist Duty Cycle

Hoist doesn’t always run at a single speed Initial acceleration - time it starts to move -

but its by the loading pocket so we don’t “floor it”

Creep 1 - carefully creeps past the loading area to avoid tearing something up

Main acceleration - after clear of loading area - hit it up to full speed

Page 44: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

44

Hoist Duty Cycle

Page 45: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

45

Duty Cycle Continued

Run at Full Speed - until you get close enough to the top that you’d better slow down or you'll put the skip up someplace interesting

Main Deceleration - slow down to creep speed before you take out the dump bin

Creep 2 - move slowly into dump position Final Deceleration - stop to dump

Page 46: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

46

What Size Motor?

Required horsepower for motor varies greatly through hoisting cycle

Adjustments are made by calculating the Root Mean Squared (RMS) Horsepower requirements

This requires taking horsepower duties at multiple points through the hoisting cycle

Page 47: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

The Spreadsheet Does Your Calculations

47

The Motor Sizing isA function of somethingCalled EEW – what isthat.?

Page 48: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

48

The Mystery of the EEW Term EEW stands for equivalent effective weight Hoist contains motors, gears, and large

wheels that contribute inertia to the system during acceleration

Could go through long hand and calculate inertia of everything (if you’re sadistic enough)

Alternative is to use manufactures tables that reduce inertia to an equivalent load on a rope.

Page 49: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

49

Nordberg Equivalent Effective Weight Chart

Page 50: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Reading the Chart

50

We know it isA Keope hoistSo I will useThe Keope line.

I know I haveA 10ft wheel

So I start at10 and read upTo the KeopeLine

Page 51: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

I Then Read Over to the Equivalent Effective Weight

51

I’ll be conservativeIn my reading andCall it 36,000 lbs

Page 52: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Enter the Number and Get MotorSizing

52

Of course understandingWhat all these HP1, HPAAnd TSL stuff is wouldAdd a lot of understanding

Page 53: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 53

The Horsepower Demand of a Keope Hoist Over Time Looks Like This

Page 54: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

54

Understanding Keope Duty Cycles

Q - Why is there a steady flat line for Horsepower required in a Keope Hoist Duty Cycle

A - Horsepower is an energy output per unit time. It takes energy to lift the skip load up the shaft as it travels at full steady speed.

Page 55: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

55

Keope Duty CyclesQ - Why is there a sloped line leading upward from when the hoist starts

A - When the hoist is operating at less than full speed the load is transported a lesser distance per unit time and thus the energy output per unit time is less. The line has a linear slope because the acceleration rate is a constant.

Page 56: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

56

The Keope Duty CycleQ - Why is there a peak that drops sharply to the flat line for Horsepower to run the Keope

A - You must add additional force to accelerate the load. At the end of the acceleration period the additional force is no longer needed.

Page 57: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

57

Keope Duty CyclesQ - Why is there a big drop in horsepower at the end of the full speed run for the hoist

A - When the hoist decelerates, the momentum of the load provides part of the energy to keep the load moving up the shaft.

Page 58: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

58

Keope CyclesQ - Why does the line slope down at the end of the Hoist Cycle

A - The load is slowing down and accumulating less potential energy per unit of time.

Page 59: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

59

Keope CyclesQ- Why the funny dashed lines that show more power being used at the start and less being recovered at the end.

A - Frictional losses

Page 60: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 60

Approach to Attacking the RMS Horsepower Requirements We will calculate components of Horsepower

requirements• HP1 will be the horsepower to accelerate the load

• HP3 will be the horsepower to move the load at full speed up the shaft

• HP2 will be the horsepower recovered from momentum when the load is decelerated

• HP6 will be the horsepower still required to lift the load after deceleration starts

• HP4 and HP5 will cover frictional losses

Page 61: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

You Can See Those Horsepowers Calculated.

61

Page 62: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 62

Horsepower #1 (For Keope Hoists) HP1 = TSL * V2 / (550 * g * Ta)

• Where TSL is the Total Suspended Load• V is the Velocity• g is the acceleration of gravity• Ta is the acceleration time to get the hoist to full

speed and includes time to accelerate to creep speed (initial acceleration t1) and then to accelerate to full speed (t3)

• Ta = t1 + t3

Page 63: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 63

Total Suspended Load TSL = EEW + 2000 * SL + 2*(2000*SW)

+ Rope Weight (both sides)• SL and SW are the skip weight and load in tons• R is the rope weight

• Because of tail rope there is a full length of rope on both skip sides

Page 64: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 64

Horsepower #3 - Power to Lift a Loaded Skip at Full Speed HP3 = V * 2000 * SL / 550

• Note that the skip weight term is missing• I have a skip going down to balance a skip

coming up

Page 65: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 65

Horsepower #2 - Negative Horsepower from Momentum During Deceleration HP2 = - TSL * V2 / (550 * g * Tr)

• Where Tr is time during deceleration

Page 66: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 66

Horsepower #4 - Losses in Gears and Drives Derived empirically rather than by physics

fundamentals HP4 = 0.111 * (2000 * SL * V / 550)

Page 67: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 67

Approach to RMS Horsepower Continued We will add the different fundamental components

of horsepower to get the horsepower needs at various cardinal points during the lift

We will label these cardinal points A through E• Example D is the peak power required at the height of

the acceleration phase

We will put the horsepower values at the cardinal points into the RMS horsepower equation and use that to size the motor.

Page 68: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 68

Calculate Horsepower at 3 Cardinal Points Point A - Peak of the Acceleration Phase HPA = HP1 + HP3 + HP4

Point B - During Full Speed Run HPB = HP3 + HP4

Point C - At Initiation of Deceleration HPC = HP2 + HP3 + HP4

Page 69: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Yip – There are the values

69

Page 70: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 70

One More Monster Power Sink

These Big Motors have an Armature to Sink a Battleship! - takes a lot of inertia to spin the thing up or down

HP5 (to spin it up) = 0.75 * HPA * 1.2 / Ta

HP6 (to spin down) = -0.75 * HPA * 1.2 / Tr

Page 71: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Those Calculations are Done Too

71

Page 72: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 72

Correcting Cardinal Points for Armature Acceleration Point D is the revision of A peak of

acceleration HPD = HPA + HP5

Point E is revision of C initiation of Deceleration

HPE = HPC + HP6

Page 73: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

And the Calculations Are There

73

Page 74: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 74

RMS Equations Depend on Motor Type For AC Motor HPrms = [ ( HPD

2 * Ta + HPB2* Tfs + HPE

2* Tr)/ ( 0.5 * Ta + Tsf + 0.5 * Tr + 0.25 * tr) ]0.5

• Where • Ta is acceleration time

• Tsf is full speed time

• Tr is deceleration time

• tr is the rest time

Page 75: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

75

RMS Horsepower for DC Motors

Numerator is the same as AC Denominator is changed to ( 0.75 * Ta + Tsf + 0.75 * Tr + 0.5 *tr)

RMS HP DC = [ Numerator/ Denominator]0.5

Page 76: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Looks Like I Need About 1200 HP

76

Page 77: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Time to Pick the Motors

77I need to choose the number and size of motor and the inertia of the rotor

Page 78: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Consider Picks

78

I’d rather go AC with frequency control. I’d like to do 2 600 hp motors butWith a 10 ft diameter Keope wheel I’ll still need gear reduction so I wouldOnly get about 94% transmission – My pick a 1250 two pole AC

Page 79: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Plug-In My Motor Parameters and Gear Reduction Efficiency

79

Ok – That seems to work(Note that there are limits to how much you can turn down the speed ofA motor with variable frequency drives)

Page 80: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Our Last Task is to Size the Brake

80

Page 81: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

We Want Two Things From Our Brake Hold the maximum possible ubalanced load

with a 1.5 factor of safety If a full speed load passes the ore dump

speed it must perform an emergency stop before the skip crashes into the top of the headframe.

81

Page 82: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

82

Next Step is to Design the Braking System During Clutching Operations the Brake must hold the

load so it doesn't go to the shaft bottom Design practice is to rate the brake and clutch to hold

the maximum load plus 50% BR = CR = (D/2) * ( 2000*SL + 2000*SW + H * Wr *

n) * (1.5) {Units are ft-lbs}• D is drum or wheel diameter• BR and CR are Brake and Clutch Ratings in ft*lbs torque • Note this is the load on one side of a drum hoist if the other is

clutched

Page 83: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

The Spreadsheet Runs the Calculation

83

I need to set my brake rating to at least this size.

Page 84: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

I Fill In the Numbers

84

Brake rating comes from the recommendationMass of the rotor came from the motor specification listThe gear ratio and speed were worked to get a workableRatio and a motor speed that was within the turn-downLimit for the motor.

Page 85: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

85

Another Factor is Brake Performance During an Emergency Stop Design is done on worst case scenario

• maximum unbalanced load traveling at full speed• discovered with a minimum tolerance distance

before you ride into the head frame or crash into the bottom

Must either design for a tolerance distance your brake can stop in or size up the brake for the tolerance you have.

Page 86: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

86

Design Concept Assume the Brake must fight against the

maximum unbalanced load• Subtract unbalanced load from brake capacity• This leaves the net force available for the

emergency stop Use Newtons Second Law

• Know the net force available• Know total mass in motion• Solve for the deceleration rate

Calculate the time and distance to stop

Page 87: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

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Formula

Look at Maximum differential load• W = (T1 - T2) * 2000

• T1 = Max load = SL + SW + (H * Wr * n/2000)

• T2 = Min Balancing Load = SW

Page 88: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

The Spreadsheet Applies the Formula to Get the Differential Weight.

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Page 89: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

89

The Mass that must be Stopped

To use Newton's Law to get Force Requirements the load must be in mass• Means we must use slugs - some how a system made by Kings using slugs

sounds wrong

M = [ ( EEW * R2 + WR2m * GR2) / R2 + T1

*2000 + T2 * 2000 ] / 32.2• Where R is the Drum or Wheel Radius D/2

• WR2m is the inertia of the motor rotor in ft2

• GR is the gear ratio of the motor to the drive• Note that the R2 terms are needed to convert rotating inertia to equivalent

mass

Page 90: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

90

Solving for the Deceleration Rate DR = ( B - W ) / M

• DR = Deceleration Rate

• M = Mass to be stopped

• W = Net unbalanced load (T1 - T2) * 2000

• B = Brake Rating in lbs linear force• Get B = BR / R

– BR is the Brake Rating in Ft*lbs

Applying the Deceleration Rate• Time to Stop = T = V / DR

• Braking Distance = S = (V/2) * T

Check Braking Distance Against Available or make sure you have the distance

Page 91: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Keope Hoist 91

The Gear Ratio Problem

GR = VM / VD• VM is rpm of motor at rated travel speed• VD is rpm of Drum

VD = V / (pi * D ) { remember I need rpm}

Page 92: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Solving for the Mass to be Stopped

Keope Hoist 92

Page 93: 1 Steps in Design of a Hoisting System ©Dr. B. C. Paul 1999 major revision 2012 With Credit to Dr. H. Sevim for Original Book

Check Out Our Stopping Distance

93

Yup – We Appear to Be OK