Fluid Mechanics
Fluid Mechanics
8th Edition
ISBN: 9781259165924
Author: Frank White
Publisher: MCGRAW-HILL HIGHER EDUCATION
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Chapter 11, Problem 11.88P
<
To determine

(a)

The type of the turbine.

<
Expert Solution
Check Mark

Answer to Problem 11.88P

Francis turbine

Explanation of Solution

Given Information:

The given table is given for water turbine having the performance data that operates with 49ft head.

Q(m3 /h) 18.7 18.7 18.5 18.3 17.6 16.7 15.1 11.5
RPM 0 500 1000 1500 2000 2500 3000 3500

η
0 14% 27% 38% 50% 65% 61% 11%

Concept Used:

Brake horse power,

bhp=ρgQHη

Q=flowH=headη=efficiencyρ=density

Calculation:

According to the equation,

bhp=ρgQHη

=62.4*0.164*49*0.65=326ft.lbf/s=0.593hp

Specified speed is given as:

Nsp=rpm*(bhp)1/2(H)5/4

=2500*(0.593)1/2(49)5/415

As, the speed with specified power is approximately 15, the type of the turbine is Francis turbine.

Conclusion:

Thus, the type of the turbine is determined.

<
To determine

(b)

To compare:

The dimensionless performance plot with the data.

<
Expert Solution
Check Mark

Answer to Problem 11.88P

The given data is different as the speed varies.

Explanation of Solution

Given Information:

The turbine which is similar has the head 150ft and the flow 6.7 ft3 /m.

Concept Used:

Brake horse power,

bhp=ρgQHη

Q=flowH=headη=efficiencyρ=density

Calculation:

The given data is different as the speed varies. The other data has the speed which is constant.

Conclusion:

Thus, the dimensionless performance plot with the data is compared.

c,d,e

To determine

The most efficient among the turbine diameter, rotation speed and horsepower.

c,d,e

Expert Solution
Check Mark

Answer to Problem 11.88P

Horse power is efficient.

Explanation of Solution

Given Information:

The given table is given for water turbine having the performance data that operates with 49ft head:

Q(m3 /h) 18.7 18.7 18.5 18.3 17.6 16.7 15.1 11.5
RPM 0 500 1000 1500 2000 2500 3000 3500

η

0 14% 27% 38% 50% 65% 61% 11%

Concept Used:

Flow coefficient,

CQ=QnD3

Head coefficient,

CH=gHn2D2

Power coefficient:

CP=Pρn3D5

Calculation:

Substituting we have:

Flow coefficient:

CQ=QnD3

=(16.73600)250060*0.08253(0.0046)41.667*0.08253=0.198

Head coefficient:

CH=gHn2D2

=9.81*49*0.3048(2500/60)20.08252=146.51(41.66)20.0825212.4

Power coefficient:

CP=Pρn3D5

=326*1.3558W998*(2500/60)30.08255=326*1.3558W998*(41.66)30.08255=1.60

With the new data the flow and head coefficients, we have:

CQ=QnD36.7904*15.73=0.198

CH=32.2*1509042*15.7212.4

P2=Cpρn23D251.60*1.94*15.13*1.315

=41000ft.lbf/s=74hp

Using the Moody step-up formula, we have:

(1η2)(1.065)/(4.84)1/4

=0.236

η2=0.764

=76.4%

So, from the new turbine the power is more than the large turbine.

P2=74hp(76%65%)

=86.5hp

87hp

Conclusion:

Thus, the most efficient among the turbine diameter, rotation speed and horsepower is determined.

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Chapter 11 Solutions

Fluid Mechanics

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