52860284 the hydraulic gradient
TRANSCRIPT
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The Hydraulic Gradient
Describes how the friction and other losses effect the Hydraulic Gradient in a pipe subjected
to a constant head
Contents
1. Introduction2. The Significance Of The Hydraulic Gradient3. The Hydraulic Gradient4. Worked Examples5. Page Comments
Introduction
In the pages on the flow of a fluid through pipes, it is seen that there is a loss of head. Whilst some of
this is due to the effect of sudden contraction or expansions in the pipe diameter, pipe fittings such as
bends and valves and entry and exit losses,a loss of potential head (i.e. The input of the pipe is higher
than the outflow) a significant portion is due to the friction in the pipe (The Darcy Equation). However
in a pipe of uniform cross section, there will be no loss of velocity head and so the loss of Total
Energy will be the result of a loss in Pressure Head. The following diagram shows a uniform pipe
and the value of pressure head at three points down its length. The line joining these points is
calledThe Hydraulic Gradient
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The Significance Of The Hydraulic Gradient
Normally when a pipe is laid, attempts are made to keep the pipe at or below the hydraulic Gradient
However in some cases this may not be possible but provided that the pipe does not rise by more than
about 26 ft. (8 mtr.) water will still flow. Above this height air comes out of solution and an airlock is
formed.
The Hydraulic Gradient
The above diagram is of an extremely simple system. On the next diagram the pipe has both a sudden
contraction and an enlargement. The various losses in energy are shown and this is used to construct
the Total Energy Line which is shown in red on the diagram.
The velocity head at the salient points in the pipe are also calculated and these are subtracted from
the Energy Line to give the Hydraulic Gradient which is shown in blue.
Worked Examples
To see the workings please click on the red buttons.
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Example 1:
Two tanks A and B are connected by a pipe 100 ft. long.
The first 70 ft. has a diameter of 3 in. and then the pipe
is suddenly reduced to 2 in. for the remaining 30 ft. The
difference of levels between the tanks is constant at 30
ft. f = 0.005 and the coefficient of contraction at all
sudden changes of area is 0.58
Find all the head losses including that at the sharp
edged pipe entry at A in terms of the velocity and
hence find the flow in gallons/min. Draw in Hydraulic
Gradient diagram.
To see the workings please click on the red button
From the diagram:-
(1)
Substituting given values
(2)
(3)
The loss at the pipe entry A
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(4)
(5)
The frictional loss along AC (The Darcy equation)
(6)
The loss caused by the sudden contraction at C
(7)
The frictional loss along CB
(8)
The velocity loss at the exit into B
=
(9)
It can be seen from the diagram that the total head lost is 8 ft. and therefore:-
(10)
(11)
The flow through the pipes is the product of the cross sectional area of the pipe and the velocity. i.e.
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(12)
(13)
Note that 1 of water wqeighs 62.4 lb. and 1 English gallon weighs 10 lbs
The Hydraulic Gradient
(14)
The velocity head in AC
(15)
The velocity head in CB
(16)
The various head losses have already been written down in terms of
It is thus now possible to tabulate actual values and enter them on a diagram of the two reservoirs
and the connecting pipes.
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The losses are:-
Entry at A 0.130 ft.
Pipe friction 1.395 ft.
Loss at C 0.657 ft.
Pipe Friction 4.550 ft.
Exit loss 1.263 ft.
The Hydraulic Gradient is the line shown in Blue
Example 2:
Two tanks, A and B are 100 ft. apart and are connected
by two pipes of 2 in. and 4 in. diameter. The height of
water in tank A is maintained at 25 ft. above that in
tank B. f = 0.008 for both pipes. The coefficient of
contraction at pipe entry is 0.585
Calculate the rate of flow in each pipe and draw the
Hydraulic Gradient. If the pipes are to be replaced by
one larger pipe, calculate the diameter of the pipe
required for the total rate of flow from A to B, to remain
unchanged.
Drawing of twin pipes from notes
To see the workings please click on the red button
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The head lost at pipe entry.
(17)Applying Bernoulli's and Darcy's equations.
(18)
For the 2 in. pipe
(19)
(20)
(21)
(22)
For the 4 in. pipe
The arithmetic is identical to that shown above except
the diameter of the pipe is now
(23)
(24)
(25)
(26)
A single pipe
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The total quantity of water flowing is
Applying Bernoulli and Darcy to the proposed pipe
(27)
(28)
(29)
But the required volume of water delivered is
(30)
(31)
Substituting in Equation (29) and solving for D
(32)
The Hydraulic Gradient for the two pipes is shown in
blue
Drawing of twin pipes modified.
Example 3:
An 8 in. diameter pipeline which connects two reservoirs
whose difference of level is 37 ft., consists of a 1000 ft.
length AB and a straight 1500 ft. length Bc having a
valve 500 ft. from the lower end C, as shown. The pipesAB and BC have each constant coefficients but BC is
slightly rougher than AB. When the flow is 600 gal./min.
a gauge at B shows that the pressure head of water is
1.7 ft. and the loss of head across the valve is 15 ft.
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Determine the maximum rate of flow if the loss of head
across the valve when fully open is 4 ft. Also draw the
Hydraulic Gradient for this quantity.
Allow for the effects of velocity head in the pipe at exit
but neglect the loss of head at pipe entry. Assume that
the horizontal projection of BC equals its length. (B.Sc.
Part1)
To see the workings please click the red button
When the flow is 600 gal./min. let the velocity of flow be and let and the the pipe friction
coefficients fo AB and BC respectively.
Thus.
(33)
Applying Bernoulli and Darcy to AB
(34)
(35)
Similarly for BC
(36)
(37)
When the flow is maximum let the velocity by
Then applying the Bernoulli and Darcy equations to the whole pipe system.
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(38)
(39)
(40)
The Hydraulic Gradient
(41)
(42)
(43)
As DC is half the length of BD
(44)
The Hydraulic gradient is shown in blue on the following diagram. Note that it has not been drawn to
scale. The difference between 37 ft. and 36.562 is due to rounding errors.
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