The question of the advisability of thus adding to a plant can only be

fairly decided when all conditions, operating and otherwise, are fully

known. For example, if we assume a large turbine to be operating on a

greatly varying load, and exhausting into a condenser, as that in Fig.

72, and, further, having an adequate stand-by to back it up, one's

obvious recommendation would be to equip the installation with both a

condenser relief valve and an atmospheric valve, in addition, of course,

to the main exhaust valve, which is always placed between the

atmospheric valve and condenser. There are still other considerations,

such as water supply, condition of circulating water, style of pump,

etc., which must all necessarily have an obvious bearing upon the

settlement of this question; so that generalization is somewhat out of

place, the final design in all cases depending solely upon general

principles and local conditions.

Other Necessary Features of a Test

In connection with the condenser, of any type, and its auxiliaries,

there remain a few necessary examinations and operations to be

conducted, if it is desired to obtain the very best results during the

test. It will be sufficient to just outline them, the method of

procedure being well known, and the requirement of any strict routine

being unnecessary. These include:

(1) A thorough examination of the air-pump, and, if possible, an equally

careful examination of diagrams taken from it when running on full

load. Also careful examination of the piping, and of any other

connections between the air pump and condenser, or other auxiliaries. It

will be well in this examination to note the general "lay" of the air

pipes, length, hight to which they rise above condenser and air pump,

facilities for drainage, etc., as this information may prove valuable in

determining the course necessary to rectify deficiencies which may later

be found to exist.

(2) In a surface condenser, inspection of the pumps delivering condensed

steam to the measuring tanks or hot-well; inspection of piping between

the condenser and the pump, and also between the pump and measuring

tanks. If these pumps are of the centrifugal type it is essential to

insure, for the purposes of a steam-consumption test, as much regularity

of delivery as possible.

(3) In the case of a consumption test upon a turbine exhausting into a

barometric condenser, and where the steam consumed is being measured by

the evaporation in the boiler over the test period, time must be devoted

to the feed-pipes between the feed-water measuring meter or tank and the

boilers. Under conditions similar to those operating in a plant such as

that shown in Fig. 72, the necessary boiler feed might be drawn from the

hot-well, the remainder of the hot-well contents probably being pumped

through water coolers, or towers, for circulating through the condenser.

With the very best system, it is possible for a slight quantity of oil

to leak into the exhaust steam, and thence to the hot-well. In its

passage, say along wooden conduits, to the measuring tank or meter, this

water would probably pass through a number of filters. The efficiency of

these must be thoroughly insured. It is unusual, in those cases where a

simple turbine steam-consumption test is being carried out, and not an

efficiency test of a complete plant, to pass the measured feed-water

through economizers. Should the latter course, owing to special

conditions, become necessary, a careful examination of all economizer

pipes would be necessary.

(4) The very careful examination of all thermometer pockets, steam- and

temperature-gage holes, etc., as to cleanliness, non-accumulation of

scale, etc.

Special Auxiliaries Necessary

Having outlined the points of interest and importance in connection with

the more permanent features of a plant, we arrive at the preparation and

fitting of those special auxiliaries necessary to carry on the test.

[Illustration: FIG. 74]

It is customary, when carrying out a first test, upon both prime mover

and auxiliaries, to place every important stage in the expansion in

communication with a gage, so that the various pressures may be recorded

and later compared with the figures of actual requirement. To do this,

in the case of the turbine, it is necessary to bore holes in the cover

leading to the various expansion chambers, and into each of these holes

to screw a short length of steam pipe, having preferably a loop in its

length, to the other end of which the gage is attached. Fig. 74

illustrates, diagrammatically, a complete turbine installation, and

shows the various points along the course taken by the steam at which it

is desirable to place pressure gages. The figure does not show the

high-pressure steam pipe, nor any of the turbine valves. With regard to

these, it will be desirable to place a steam gage in the pipe,

immediately before the main stop-valve, and another immediately after

it. Any fall of pressure between the two sides of the valve can thus be

detected. To illustrate this clearly, Fig. 75 is given, showing the

valves of a turbine, and the position of the gages connected to them.

The two gages E and F on either side of the main stop-valve A are also

shown. The steam after passing through the valve, which, in the case of

small turbines, is hand-operated, goes in turn through the automatic

stop-valve B, the function of which is to automatically shut steam off

should the turbine attain a predetermined speed above the normal, the

steam strainer C, and finally through the governing valve D into the

turbine. As shown, gages G and H are also fitted on either side of the

strainer, and these, in conjunction with gages E and F, will enable any

fall in pressure between the first two valves and the governing valve to

be found. Up to the governing-valve inlet no throttling of the steam

ought to take place under normal conditions, i.e., with all valves open,

and consequently any fall in pressure between the steam inlet and this

point must be the result of internal wire-drawing. By placing the gages

as shown, the extent to which this wire-drawing affects the pressures

obtainable can be discovered.

[Illustration: FIG. 75]

On varying and even on normal and steady full load, the steam is more or

less reduced in pressure after passing through the governing valve D; a

gage I must consequently be placed between the valve, preferably on the

valve itself, and the turbine. Returning to Fig. 74, the gages shown are

A, B, C, D, and E, connected to the first, second, third, fourth, and

fifth expansions; also F in the turbine and exhaust space, where there

are no blades, G in the exhaust pipe immediately before the main exhaust

valve E (see Fig. 73), and H connected to the condenser. On condensing

full load it is probable that A, B, and C will all register pressures

above the atmosphere, while gages D, E, F, and G will register pressures

below the atmosphere, being for this purpose vacuum gages. On the other

hand, with a varying load, and consequently varying initial pressures,

one or two of the gages may register pressure at one moment and vacuum

at another. It will therefore be necessary to place at these points

compound gages capable of registering both pressure and vacuum. With the

pressures in the various stages constantly varying, however, a gage is

not by any means the most reliable instrument for recording such

variations. The constant swinging of the finger not only renders

accurate reading at any particular moment both difficult and, to an

extent, unreliable, but, in addition, the accompanying sudden changes of

condition, both of temperature and pressure, occurring inside the gage

tube, in a comparatively short time permanently warp this part, and thus

altogether destroy the accuracy of the gage. It is well known that even

with the best steel-tube gages, registering comparatively steady

pressures, this warping of the tube inevitably takes place. The quicker

deterioration of such gage tubes, when the gage is registering quickly

changing pressures, can therefore readily be conceived, and for this

reason alone it is desirable to have all gages, whatever the conditions

under which they work, carefully tested and adjusted at short intervals.

If it is desired to obtain reliable registration of the several

pressures in the different expansions of a turbine running on a varying

load, it would therefore seem advisable to obtain these by some type of

external spring gage (an ordinary indicator has been found to serve well

for this purpose) which the sudden internal variations in pressure and

temperature cannot deleteriously affect.

In view of the great importance he must attach to his gage readings, the

tester would do well to test and calibrate and adjust where necessary

all the gages he intends using during a test. This he can do with a

standard gage-testing outfit. By this means only can he have full

confidence in the accuracy of his results.

In like manner it is his duty personally to supervise the connecting and

arrangement of the gages, and the preliminary testing for leakage which

can be carried out simultaneously with the vacuum test made upon the

turbine casing.

Where Thermometers are Required

Equally important with the foregoing is the necessity of calibrating and

testing of all thermometers used during a test. Where possible it is

advisable to place new thermometers which have been previously tested

at all points of high temperature. Briefly running them over, the points

at which it is necessary to place thermometers in the entire system of

the steam and condensing plant are as follows:

(1) A thermometer in the steam pipe on the boiler, where the pipe leaves

the superheater.

(2) In the steam pipe immediately in front of the main stop-valve, near

point E in Fig. 75.

(3) In the main governing valve body (see I, Fig. 75) on the inlet side.

(4) In the main governing valve body on the turbine side, which will

register temperatures of steam after it has passed through the valve.

(5) In the steam-turbine high-pressure chamber, giving the temperature

of the steam before it has passed through any blades.

(6) In the exhaust chamber, giving the temperature of steam on leaving

the last row of blades.

(7) In the exhaust pipe near the condenser.

(8) In the condenser body.

(9) In the circulating-water inlet pipe close to the condenser.

(10) In the circulating-water outlet pipe close to the condenser.

(11) In the air-pump suction pipe close to the condenser.

(12) In the air-pump suction pipe close to the air pump.

It is not advisable to place at those vital points, the readings at

which directly or indirectly affect the consumption, two thermometers,

say one ordinary chemical thermometer and one thermometer of the gage

type, thus eliminating the possibility of any doubt which might exist

were only one thermometer placed there.

There is no apparent reason why one should attempt to take a series of

temperature readings during a consumption test on varying load. The

temperatures registered under a steady load test can be obtained with

great reliability, but on a varying load, with constantly changing

temperatures at all points, this is impossible. This is, of course,

owing to the natural sluggishness of the temperature-recording

instruments, of whatever class they belong to, in responding to changes

of condition. As a matter of fact, the possibility of obtaining

correctly the entire conditions in a system running under greatly

varying loads is very doubtful indeed, and consequently great reliance

cannot be placed upon figures obtained under such conditions.

A few simple calculations will reveal to the tester his special

requirements in the direction of measuring tanks, piping, etc., for his

steam consumption test. Thus, assuming the turbine to be tested to be of

3000 kilowatt capacity normal load, with a guaranteed steam consumption

of, say, 14.5 pounds per kilowatt-hour, he calculates the total water

rate per hour, which in this case would be 43,500 pounds, and designs

his weighing or measuring tanks to cope with that amount, allowing, of

course, a marginal tank volume for overload requirements.

VIII. TROUBLES WITH STEAM TURBINE AUXILIARIES[7]

[7] Contributed to _Power_ by Walter B. Gump.

The case about to be described concerns a steam plant in which there

were seven cross-compound condensing Corliss engines, and two Curtis

steam turbines. The latter were each of 1500-kilowatt capacity, and were

connected to surface condensers, dry-vacuum pumps, centrifugal, hot-well

and circulating pumps, respectively. In the illustration (Fig. 76), the

original lay-out of piping is shown in full lines. Being originally a

reciprocating plant it was difficult to make the allotted space for the

turbines suitable for their proper installation. The trouble which

followed was a perfectly natural result of the failure to meet the

requirements of a turbine plant, and the description herein given is but

one example of a great many where the executive head of a concern

insists upon controlling the situation without regard to engineering

advice or common sense.

[Illustration: FIG. 76. TURBINE AUXILIARIES AND PIPING]

Circulating Pump Fails to Meet Guarantee

Observing the plan view, it will be seen that the condensers for both

turbines receive their supply of cooling water from the same supply

pipe; that is, the pipes, both suction and discharge, leading to No. 1

condenser are simply branches from No. 2, which was installed first

without consideration for a second unit. When No. 1 was installed there

was a row of columns from the basement floor to the main floor extending

in a plane which came directly in front of the condenser. The column P

shown in the plan was so located as to prevent a direct connection

between the centrifugal circulating pump and the condenser inlet. The

centrifugal pump was direct-connected to a vertical high-speed engine,

and the coupling is shown at E in the elevation.

Every possible plan was contemplated to accommodate the engine and pump

without removing any of the columns, and the arrangement shown was

finally adopted, leaving the column P in its former place by employing

an S-connection from the pump to the condenser. It should be stated that

the pump was purchased under a guarantee to deliver 6000 gallons per

minute under a head of 50 feet, with an impeller velocity of 285

revolutions per minute. The vertical engine to which the pump was

connected proved to be utterly unfit for running at a speed beyond 225

to 230 revolutions per minute, and in addition the S-bend would

obviously reduce the capacity, even at the proper speed of the impeller.

Besides these factors there was another feature even more serious. It

was found that when No. 2 unit was operating No. 1 could not get as

great a quantity of circulating water as when No. 2 was shut down. This

was because No. 2 was drawing most of the water, and No. 1 received only

that which No. 2 could not pull from the suction pipe A. This will be

clear from the fact that the suction and discharge pipes for No. 1 were

only 16 inches, while those of No. 2 were 20 inches and 16 inches,

respectively. The condenser for No. 2 had 1000 square feet less cooling

surface than No. 1, which had 6000 square feet and was supplied with

cooling water by means of two centrifugal pumps of smaller capacity

than for No. 1 and arranged in parallel. These were each driven by an

electric motor, and were termed "The Siamese Twins," due to the way in

which they were connected.

The load factor of the plant ranged from 0.22 to 0.30, the load being

almost entirely lighting, so that for the winter season the load factor

reached the latter figure. The day load was, therefore, light and not

sufficient to give one turbine more than from one-fourth to one-third

its rated capacity. Under these conditions No. 1 unit was able to

operate much more satisfactorily than when fully loaded, because of the

fact that the cooling water was more effective. This was, of course, all

used by No. 1 unit when No. 2 was not operating. At best, however, it

was found that the vacuum could not be made to exceed 24 inches, and

during the peak, with the two turbines running, the vacuum would often

drop to 12 inches. A vacuum of 16 inches or 18 inches on the peak was

considered good.

An Investigation

Severe criticism "rained" heavily upon the engineer in charge, and

complaints were made in reference to the high oil consumption. An

investigation on the company's part followed, and the firm which

furnished the centrifugal pump and engine was next in order to receive

complaints. Repeated efforts were made to increase the speed of the

vertical engine to 285 revolutions per minute, but such a speed proved

detrimental to the engine, and a lower speed of about 225 revolutions

per minute had to be adopted.

A thorough test on the pump to ascertain its delivery at various speeds

was the next move, and a notched weir, such as is shown in the

elevation, was employed. The test was made on No. 2 cooling tower, not

shown in the sketch, and showed that barely 3000 gallons per minute were

being delivered to the cooling tower. While the firm furnishing the pump

was willing to concede that the pump might not be doing all it should,

attention was called to the fact that there might be some other

conditions in connection with the system which were responsible for the

losses. Notable among these was the hydraulic friction, and when this

feature of the case was presented, the company did not seem at all

anxious to investigate the matter further; obviously on account of

facing a possible necessity for new piping or other apparatus which

might cost something.

Approximately 34 feet was the static head of water to be pumped over No.

2 cooling tower. Pressure gages were connected to the suction,

discharge, and condenser inlet, as shown at G, G' and G'' respectively.

When No. 1 unit was operating alone the gage G showed practically zero,

indicating no vacuum in the suction pipe. Observing the same gage when

No. 2 unit was running, a vacuum as high as 2 pounds was indicated,

showing that No. 2 was drawing more than its share of cooling water from

the main A and hence the circulating pump for No. 1 was fighting for all

it received. Gage G' indicated a pressure of 21 pounds, while G''

indicated 18.5 pounds, showing a difference of 2.5 pounds pressure lost

in the S-bend. This is equivalent to a loss of head of nearly 6 feet,

0.43 pound per foot head being the constant employed. The total head

against which the pump worked was therefore

G' + G = 21 + 2,

or

23

---- = 53

0.43

feet approximately. Since the static head was 34 feet, the head lost in

friction was evidently

53-34 = 19

feet, or

1900

---- = 36

53

per cent., approximately.

Supply of Cooling Water Limited

In addition to this the supply of cooling water was limited, the vacuum

being extremely low at just the time when efficient operation should be

had. The natural result occurred, which was this: As the load on the

turbine increased, the amount of steam issuing into the condenser

increased, beating [Transcriber: heating?] the circulating water to a

temperature which the cooling tower (not in the best condition) was

unable to decrease to any great extent. The vacuum gradually dropped

off, which indicated that the condenser was being filled with vapor, and

in a short time the small centrifugal tail-pump lost its prime,

becoming "vapor bound," and the vacuum further decreased. The steam

which had condensed would not go into the tail-pump because of the

tendency of the dry-pump to maintain a vacuum. When a certain point was

reached the dry-vacuum pump started to draw water in its cylinder, and

the unit had to be shut down immediately.

Vapor-bound Pumps

As the circulating water gradually rose in temperature the circulating

pump also became "vapor bound," so that the unit would be tied up for

the rest of the night, as this pump could not be made to draw hot water.

The reason for this condition may be explained in the following way.

When the circulating pump was operating and there was a suction of 2

pounds indicated at G, the water was not flowing to the pump of its own

accord, but was being pulled through by force. This water would flow

through the pump until a point was reached when the water became hot

enough to be converted into vapor, this occurring at a point where the

pressure was sufficiently reduced to cause the water to boil. Naturally

this point was in the suction pipe and vapor was thus maintained behind

the pump as long as it was operating. In this case the pump was merely

maintaining a partial vacuum, but not drawing water. After the vacuum

was once lost, by reason of the facts given, it could not be regained,

as the circulating water, piping and condenser required a considerable

period of time in which to cool.

Before any radical changes were made it was decided that a man should

crawl in the suction pipe A, and remove such sand, dirt, or any other

obstacles as were believed to cause the friction. After this had been

done and considerable sand had been removed, tests were resumed with

practically the same results as before. The investigation was continued

and the dry-vacuum pumps were overhauled, as they had been damaged by

water in the cylinders, and furthermore needed re-boring. In short, the

auxiliaries were restored to the best condition that could be brought

about by the individual improvement of each piece of apparatus. As this

was not the seat of the trouble, however, the remedy failed to effect a

"cure." It was demonstrated that the steam consumption of the turbines

was greatly increased due to priming of the boilers, as well as

condensation in the turbine casing; hence, the ills above mentioned were

aggravated.

Changes in Piping

After a great deal of argument from the chief engineer, and the firm

which furnished the pump, both making a strong plea for a change in the

piping, the company accepted the inevitable, and the dotted portion

shows the present layout. The elbow M was removed, and a tee put in its

place to which the piping D was connected. The circulating pump was

removed to the position shown, and a direct connection substituted for

the S-bend. The discharge pipe C was carried from No. 1 unit separately,

as shown in the elevation, and terminated at No. 1 cooling tower

instead of No. 2, which shortened the distance about 60 feet, the total

length of pipe (one way) from No. 1 unit being originally 250 feet. In

this way the condensing equipment was made practically separate for each

turbine, as it should have been in the first place.

With the new piping a vacuum of 24 inches on the peak could be reached.

While this is far from an efficient value, yet it is better than the

former figure. The failure to reach a vacuum of 28 inches or better is

due primarily to a lack of cooling water, but an improvement in this

regard could be made by reconstructing the cooling towers, which at

present do not offer the proper amount of cooling surface. The screens

used were heavy galvanized wire of about 3/16-inch mesh, which became

coated in a short time, and must be thoroughly cleaned to permit the

water to drop through them. The supply of cooling water was taken from a

30-inch pipe line several miles long and fed from a spring. The amount

of water varied considerably and was at times quite insufficient for the

load on the plant. Instead of meeting this condition with the best

apparatus possible, a chain of difficulties were added to it, with the

results given.

INDEX

Acceleration, rate of, 147

Adjustment, axial, 65

making, 66

Air-pump, examining, 163

Allis-Chalmers Co. steam turbine, 41

Auxiliaries, 2, 154

special, 165

Auxiliary plant for consumption test, 137

spring on governor dome, 28

Axial adjustment, 65

Baffler, 36

functions, 39

Bearings, main, 69

Blades, construction details, 44

inspecting, 104

Blading, Allis-Chalmers turbine, 48

Westinghouse-Parsons turbine, 59, 92

Blueprints, studying, 11

Buckets, moving, 14

stationary, 14

Bushings, 36

Carbon packing, 19

ring, 20

Central gravity oiling system, 111

Circulating pump fails to meet guarantee, 172

Clearance, 15, 150

adjusting, 18

between moving and stationary buckets, 4

gages, 17

measuring, 18

radial, 63

Comma lashing, 95

Condensers, 108, 131

jet, 154

Conditions for successful operation, 105

Cooling water supply limited, 177

Coupling, 127

Cover-plate, 4

-plate, lowering, 9

Curtis turbine, 11

turbine in practice, 1

setting valves, 31, 32

De Laval turbines, 118

Draining system, 105

Dummy leakage, 115

pistons, 63, 65

rings, 43, 113, 114

Equalizing pipes, 64

Exhaust end of turbine, 107

pipe, 107

Expanding nozzles, 14

Feed-pipes, 164

Flow, rate, 38

Foundation drawings, 2

rings, 44, 46

Fourth-stage wheel, 14

Franklin, Thomas, 112, 137, 154

Gages, calibrating and adjusting, 169

clearance, 17

for test work, 165

Generator, 53

Glands, examination for scale, 104

packing, 71, 77

regulation, 148

Steam Turbines A Book of Instruction for the Adjustment and Operation of the Principal Types of this Class of Prime Movers · 第 7 / 8 段