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based on the lecture notes and the textbook to finish the homework, write step by step!.testbook:http://libgen.io/ads.php?md5=46EAA9C37C0DBCB9E7A1CD7C6625F91A Problems: (4 points each, unless...

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based on the lecture notes and the textbook to finish the homework, write step by step!.testbook:http://libgen.io/ads.php?md5=46EAA9C37C0DBCB9E7A1CD7C6625F91A
Problems: (4 points each, unless otherwise noted)
1. Problem 5.76
2. Problem 5.81
3. Problem 3.20
4. Problem 3.24 The required suction pressure is P3 where point 3 is on the wing. Point 2 is a
stagnation point at the leading edge of the wing. The velocity at point 2 (and at any stagnation
point) is zero. The pressure at point 2 is a stagnation pressure P 0 2 .
5. Problem 3.32
6. Problem 3.48 Hint: The lowest pressure in the tube (e.g, the point where the tube will collapse)
is at the top of the U in the tube.
7. Problem 3.54
8. Problem 3.61
9. Problem 3.67
Answered Same Day Dec 26, 2021

Solution

David answered on Dec 26 2021
115 Votes
Ans. 5.81
As shown in the above diagrame, there is a pump which is pumping the fluid from the lake to the
eservoir, so calculate the power of the pump required to reach the water in the reservoir,
Apply the Bernoulli’s principle at the lake point and the reservoir point,
So,
2
1 1 2 2
1 2
1 1 1
2
2 2
0, 0, 0
20
p L
P v P V
Z h h Z
g r g
where P Z V
Z ft

      
  


So put the values in the above equation,
So,
2
2p L
P
h h Z
  
Calculate the rate of flow of water, and convert the unit,
3
3
1000 1 1
( ) ( )
10min 7.48 60
0.223
gal ft
Q
gal
Q ft s
 
   
 


Now,
2
1
3 550
119
62.4 0.223
2 2 14.7 144
4230
20 87.8
62.4
,
87.8 119 87.8 31.2
p
p
p L L
p
W
h ft
Q
If P atm
h h h ft
Thus if
h h ft ft
ï‚´
  
ï‚´
   
    
    

The given pump will work for P=2atm
2 2
3 6350 ,
6350
20 122
62.4
p L L
If
l
P atm then
ft
h h h
 
    

Thus, If this pump is to work
119 122
3
L
L
ft h ft
h ft
 
 

Since it is not possible to have 0Lh  Thus pump will not work for 2 3P atm .
Ans 3.61
Apply Bernoulli’s principle at both the points,
2 2
1 1 2 2
1 2
2 1
1
2 2
,
( )
2
P V P V
Z Z
g r g
So
P P
V g
    



Here the total height term applies for the equili
ium,
So,
1 2
2 1
( )
( )
m
m
P rl r h P r l h
P P r r h
    
  

Put the value in the equation (1)
2
3
2
3
3
( )
2
1.07 9.8 10
2(9.81)( 1)0.02
10.49
3.99 10 1
,
mr rV g h
V m
apply thecantinuety principle
Q AV
Q
here r is kN m



ï‚´ ï‚´
 

  
...
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