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-4dvirtiendo que la potencia P es<br />

(32) P = rjyQH<br />

donde q es la eficiencia y la tasa de flujc Q la<br />

produce:<br />

(33)<br />

ndj2<br />

Q = Vj 4 =<br />

ndj2<br />

CVG y-<br />

entonces la veiocidad especifica de la mhquina es<br />

(34) N,=<br />

o, aproximadamente,<br />

(35)<br />

dj<br />

2114 Gig D<br />

(9<br />

N, = 1.3 D<br />

Asi, pues, la velocidad cspecifica es, aproximada-<br />

ment.e, 1, 3 veces la relaci6n de1 digmetro de1 chorro<br />

al diametro de la rueda. Los valores prkticos de<br />

dj/D para las ruedas Pelton osciian entre 0,04 y 0,3.<br />

lo que significa que N, estara en la gama de 0,05 a<br />

0,13 (19 a 25 en unidades m&ricas). En ias turbinas<br />

Turgo, ei digmetro reiativo de !a rueda puede ser la<br />

mitad que el de una rueda Pelton, 10 que produce<br />

veiocidades especificas de aproximadamente el .dobie,<br />

de !as de disefio conventional. Son posibles<br />

velocidades especificas m&s elevadas con disefios de<br />

inyectores mtitiples. El aumento es proporcionai a la<br />

raiz cuadrada de1 ntimero de inyectores.<br />

multiple nozzle designs. The increase is propor-<br />

tional to the square root of the number of<br />

nozzles.<br />

Reaction Turbines. The main difference bet-<br />

ween impulse wheels and reaction turbines is the<br />

fact that a pressure drop takes place in the<br />

rotating passages. This implies that the entire<br />

flow passage from turbine in!et to discharge a?<br />

the tailwater must be <strong>com</strong>pletely fiiied. Typicai<br />

turbine runners are illustrated in Fig. 6.<br />

The specific speed range for reaction wheels is<br />

much broader than for impulse wheels. A typical<br />

installation is sketched. (Figure 14)<br />

The main difference is the draft tube which is<br />

considered an integral part of the machine. Its<br />

main functions are to allow a turbine setting<br />

above the tailwater without a reduction in net<br />

head and to reduce the head loss at the<br />

submerged discharge by diffusing the flow leav-<br />

ing the turbine.<br />

In an impulse wheel, the head represented by<br />

setting the turbine above the tailwater is lost,<br />

but, since impulse wheels are generally operated<br />

at high head, this represents a small fraction of<br />

the total head available. Referring to the diagram,<br />

the head available to the runner is<br />

P4- v212 v2 - Vd2<br />

(36) H’= H-kD 3n - 3n<br />

DiFfuser Sudden<br />

Loss Enlargement<br />

Turbinas de Reaccih. La principal diferencia en- Basically two losses are associated with the<br />

tre las ruedas de impuisos y ias turbinas de reacci6n draft tube; viscous losses within the draft tube<br />

se debe a que en 10s pasajes de rotaci6n se produce associated with flow diffusion and external mixuna<br />

rcducci6n de la presi6n. Esto significa que todo ing losses associated with the discharge into the<br />

el pasaje de1 flujo desde la entrada de la turbina a la tailwater. Obviously, the first loss can be<br />

descarga en el agua de descarga el tubo ha de estar minimized by reducing the amount of diffusion at<br />

<strong>com</strong>pletamente lleno. En la figura 6 se ilustran the expense of increased outlet losses.<br />

rotores tipicos de turbina. As an illustration of the design and operation<br />

La gama de velocidades especificas para 10s ruedos<br />

of turbines for constant speed, refer again to Fig.<br />

de reacci6n es mucho m8s amplia que para 10s rueda 1. The pivoted guide vanes allow for control of<br />

de impulsos. A continuaci6n esbozamos una instala- the magnitude and direction of Vl, ie. V1 and al.<br />

cidn tipica. (Figura 14) The relationship between blade angle, inlet<br />

velocity, and peripheral speed is<br />

La principal diferencia radica en la galeria de suc-<br />

ci6n que se considera <strong>com</strong>a una parte integral de la<br />

mgquina. Sus principales funciones consisten en permitir<br />

la instalacidn de la turbina por encima de1 agua<br />

de descarga sin reducir la caida neta y reducir la (37)<br />

p6rdida de la caida en la descarga sumergida<br />

mediante la difusi6n de1 flujo que sale de la turbina.<br />

137<br />

cot /3, =<br />

VI cos q-U1<br />

VI sin al

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