- Source: Blade element theory
Blade element theory (BET) is a mathematical process originally designed by William Froude (1878), David W. Taylor (1893) and Stefan Drzewiecki (1885) to determine the behavior of propellers. It involves breaking a blade down into several small parts then determining the forces on each of these small blade elements. These forces are then integrated along the entire blade and over one rotor revolution in order to obtain the forces and moments produced by the entire propeller or rotor. One of the key difficulties lies in modelling the induced velocity on the rotor disk. Because of this the blade element theory is often combined with momentum theory to provide additional relationships necessary to describe the induced velocity on the rotor disk, producing blade element momentum theory. At the most basic level of approximation a uniform induced velocity on the disk is assumed:
v
i
=
T
A
⋅
1
2
ρ
.
{\displaystyle v_{i}={\sqrt {{\frac {T}{A}}\cdot {\frac {1}{2\rho }}}}.}
Alternatively the variation of the induced velocity along the radius can be modeled by breaking the blade down into small annuli and applying the conservation of mass, momentum and energy to every annulus. This approach is sometimes called the Froude–Finsterwalder equation.
If the blade element method is applied to helicopter rotors in forward flight it is necessary to consider the flapping motion of the blades as well as the longitudinal and lateral distribution of the induced velocity on the rotor disk. The most simple forward flight inflow models are first harmonic models.
Simple blade element theory
While the momentum theory is useful for determining ideal efficiency, it gives a very incomplete account of the action of screw propellers, neglecting among other things the torque. In order to investigate propeller action in greater detail, the blades are considered as made up of a number of small elements, and the air forces on each element are calculated. Thus, while the momentum theory deals with the flow of the air, the blade-element theory deals primarily with the forces on the propeller blades. The idea of analyzing the forces on elementary strips of propeller blades was first published by William Froude in 1878. It was also worked out independently by Drzewiecki and given in a book on mechanical flight published in Russia seven years later, in 1885. Again, in 1907, Lanchester published a somewhat more advanced form of the blade-element theory without knowledge of previous work on the subject. The simple blade-element theory is usually referred to, however, as the Drzewiecki theory, for it was Drzewiecki who put it into practical form and brought it into general use. Also, he was the first to sum up the forces on the blade elements to obtain the thrust and torque for a whole propeller and the first to introduce the idea of using airfoil data to find the forces on the blade elements.
In the Drzewiecki blade-element theory the propeller is considered a warped or twisted airfoil, each segment of which follows a helical path and is treated as a segment of an ordinary wing. It is usually assumed in the simple theory that airfoil coefficients obtained from wind tunnel tests of model wings (ordinarily tested with an aspect ratio of 6) apply directly to propeller blade elements of the same cross-sectional shape.
The air flow around each element is considered two-dimensional and therefore unaffected by the adjacent parts of the blade. The independence of the blade elements at any given radius with respect to the neighbouring elements has been established theoretically and has also been shown to be substantially true for the working sections of the blade by special experiments made for the purpose. It is also assumed that the air passes through the propeller with no radial flow (i.e., there is no contraction of the slipstream in passing through the propeller disc) and that there is no blade interference.
= Aerodynamic forces on a blade element
=Consider the element at radius r, shown in Fig. 1, which has the infinitesimal length dr and the width b. The motion of the element in an aircraft propeller in flight is along a helical path determined by the forward velocity V of the aircraft and the tangential velocity 2πrn of the element in the plane of the propeller disc, where n represents the revolutions per unit time. The velocity of the element with respect to the air Vr is then the resultant of the forward and tangential velocities, as shown in Fig. 2. Call the angle between the direction of motion of the element and the plane of rotation Φ, and the blade angle β. The angle of attack α of the element relative to the air is then
α
=
β
−
ϕ
{\displaystyle \alpha =\beta -\phi }
.
Applying ordinary airfoil coefficients, the lift force on the element is:
d
L
=
1
2
V
r
2
C
L
b
d
r
.
{\displaystyle dL={\frac {1}{2}}V_{r}^{2}C_{L}b\,dr.}
Let γ be the angle between the lift component and the resultant force, or
γ
=
arctan
D
L
{\textstyle \gamma =\arctan {\frac {D}{L}}}
. Then the total resultant air force on the element is:
d
R
=
1
2
V
r
2
C
L
b
d
r
cos
γ
.
{\displaystyle dR={\frac {{\frac {1}{2}}V_{r}^{2}C_{L}b\,dr}{\cos \gamma }}.}
The thrust of the element is the component of the resultant force in the direction of the propeller axis (Fig. 2), or
d
T
=
d
R
cos
(
ϕ
+
γ
)
=
1
2
V
r
2
C
L
b
cos
(
ϕ
+
γ
)
cos
γ
d
r
,
{\displaystyle {\begin{aligned}dT&=dR\cos(\phi +\gamma )\\&={\frac {{\frac {1}{2}}V_{r}^{2}C_{L}b\cos(\phi +\gamma )}{\cos \gamma }}dr,\end{aligned}}}
and since
V
r
=
V
sin
ϕ
{\textstyle V_{r}={\frac {V}{\sin \phi }}}
d
T
=
1
2
V
2
C
L
b
cos
(
ϕ
+
γ
)
sin
2
ϕ
cos
γ
d
r
.
{\displaystyle dT={\frac {{\frac {1}{2}}V^{2}C_{L}b\cos(\phi +\gamma )}{\sin ^{2}\phi \cos \gamma }}dr.}
For convenience let
K
=
C
L
b
sin
2
ϕ
cos
γ
{\displaystyle K={\frac {C_{L}b}{\sin ^{2}\phi \cos \gamma }}}
and
T
c
=
K
cos
(
ϕ
+
γ
)
.
{\displaystyle T_{c}=K\cos(\phi +\gamma ).}
Then
d
T
=
1
2
ρ
V
2
T
c
d
r
,
{\displaystyle dT={\frac {1}{2}}\rho V^{2}T_{c}\,dr,}
and the total thrust for the propeller (of B blades) is:
T
=
1
2
ρ
V
2
B
∫
0
R
T
c
d
r
.
{\displaystyle T={\frac {1}{2}}\rho V^{2}B\int _{0}^{R}T_{c}\,dr.}
Referring again to Fig. 2, the tangential or torque force is
d
F
=
d
R
sin
(
ϕ
+
γ
)
,
{\displaystyle dF=dR\sin(\phi +\gamma ),}
and the torque on the element is
d
Q
=
r
d
R
sin
(
ϕ
+
γ
)
,
{\displaystyle dQ=r\,dR\,\sin(\phi +\gamma ),}
which, if
Q
c
=
K
r
sin
(
ϕ
+
γ
)
{\textstyle Q_{c}=Kr\sin(\phi +\gamma )}
, can be written
d
Q
=
1
2
ρ
V
2
Q
c
d
r
.
{\displaystyle dQ={\frac {1}{2}}\rho V^{2}Q_{c}dr.}
The expression for the torque of the whole propeller is therefore
Q
=
1
2
ρ
V
2
B
∫
0
R
Q
c
d
r
.
{\displaystyle Q={\frac {1}{2}}\rho V^{2}B\int _{0}^{R}Q_{c}dr.}
The horsepower absorbed by the propeller, or the torque horsepower, is
Q
H
P
=
2
π
n
Q
550
{\displaystyle QHP={\frac {2\pi nQ}{550}}}
and the efficiency is
η
=
T
H
P
Q
H
P
=
T
V
2
π
n
Q
.
{\displaystyle \eta ={\frac {THP}{QHP}}={\frac {TV}{2\pi nQ}}.}
= Efficiency
=Because of the variation of the blade width, angle, and airfoil section along the blade, it is not possible to obtain a simple expression for the thrust, torque, and efficiency of propellers in general. A single element at about two-thirds or three-fourths of the tip radius is, however, fairly representative of the whole propeller, and it is therefore interesting to examine the expression for the efficiency of a single element. The efficiency of an element is the ratio of the useful power to the power absorbed, or
η
=
d
T
V
d
Q
2
π
n
=
d
R
cos
(
ϕ
+
γ
)
V
d
R
sin
(
ϕ
+
γ
)
2
π
n
r
=
tan
ϕ
tan
(
ϕ
+
γ
)
.
{\displaystyle {\begin{aligned}\eta &={\frac {dTV}{dQ2\pi n}}\\&={\frac {dR\cos(\phi +\gamma )V}{dR\sin(\phi +\gamma )2\pi nr}}\\&={\frac {\tan \phi }{\tan(\phi +\gamma )}}.\end{aligned}}}
Now tan Φ is the ratio of the forward to the tangential velocity, and
tan
γ
=
D
L
{\textstyle \tan \gamma ={\frac {D}{L}}}
. According to the simple blade-element theory, therefore, the efficiency of an element of a propeller depends only on the ratio of the forward to the tangential velocity and on the
D
L
{\textstyle {\frac {D}{L}}}
of the airfoil section.
The value of Φ which gives the maximum efficiency for an element, as found by differentiating the efficiency with respect to Φ and equating the result to zero, is
ϕ
=
45
∘
−
γ
2
{\displaystyle \phi =45^{\circ }-{\frac {\gamma }{2}}}
The variation of efficiency with 0 is shown in Fig. 3 for two extreme values of γ. The efficiency rises to a maximum at
45
∘
−
γ
2
{\textstyle 45^{\circ }-{\frac {\gamma }{2}}}
and then falls to zero again at
90
∘
−
γ
{\textstyle 90^{\circ }-\gamma }
. With an
L
D
{\textstyle {\frac {L}{D}}}
of 28.6 the maximum possible efficiency of an element according to the simple theory is 0.932, while with an
L
D
{\textstyle {\frac {L}{D}}}
of 9.5 it is only 0.812. At the values of Φ at which the most important elements of the majority of propellers work (10° to 15°) the effect of
L
D
{\textstyle {\frac {L}{D}}}
on efficiency is still greater. Within the range of 10° to 15°, the curves in Fig. 3 indicate that it is advantageous to have both the
L
D
{\textstyle {\frac {L}{D}}}
of the airfoil sections and the angle Φ (or the advance per revolution, and consequently the pitch) as high as possible.
= Limitations
=According to momentum theory, a velocity is imparted to the air passing through the propeller, and half of this velocity is given the air by the time it reaches the propeller plane. This increase of velocity of the air as it passes into the propeller disc is called the inflow velocity. It is always found where there is pressure discontinuity in a fluid. In the case of a wing moving horizontally, the air is given a downward velocity, as shown in Fig. 4., and theoretically half of this velocity is imparted in front of and above the wing, and the other half below and behind.
This induced downflow is present in the model wing tests from which the airfoil coefficients used in the blade-element theory are obtained; the inflow indicated by the momentum theory is therefore automatically taken into account in the simple blade-element theory. However, the induced downflow is widely different for different aspect ratios, being zero for infinite aspect ratio. Most model airfoil tests are made with rectangular wings having an arbitrarily chosen aspect ratio of 6, and there is no reason to suppose that the downflow in such a test corresponds to the inflow for each element of a propeller blade. In fact, the general conclusion drawn from an exhaustive series of tests, in which the pressure distribution was measured over 12 sections of a model propeller running in a wind tunnel, is that the lift coefficient of the propeller blade element differs considerably from that measured at the same angle of attack on an airfoil of aspect ratio 6. This is one of the greatest weaknesses of the simple blade-element theory.
Another weakness is that the interference between the propeller blades is not considered. The elements of the blades at any particular radius form a cascade similar to a multiplane with negative stagger, as shown in Fig. 5. Near the tips where the gap is large the interference is very small, but in toward the blade roots it is quite large.
In actual propellers there is a tip loss which the blade-element theory does not take into consideration. The thrust and torque forces as computed by means of the theory are therefore greater for the elements near the tip than those found by experiment.
In order to eliminate scale effect, the wind tunnel tests on model wings should be run at the same value of Reynolds number (scale) as the corresponding elements in the propeller blades. Airfoil characteristics measured at such a low scale as, for example, an air velocity of 30 m.p.h. with a 3-in. chord airfoil, show peculiarities not found when the tests are run at a scale comparable with that of propeller elements. The standard propeller section characteristics given in Figs. 11, 12, 13, and 14 were obtained from high Reynolds-number tests in the Variable Density Tunnel of the NACA, and, fortunately, for all excepting the thickest of these sections there is very little difference in characteristics at high and low Reynolds numbers. These values may be used with reasonable accuracy as to scale for propellers operating at tip speeds well below the speed of sound in air, and therefore relatively free from any effects of compressibility.
The poor accuracy of the simple blade-element theory is very well shown in a report by Durand and Lesley, in which they have computed the performance of a large number of model propellers (80) and compared the computed values with the actual performances obtained from tests on the model propellers themselves. In the words of the authors: The divergencies between the two sets of results, while showing certain elements of consistency, are on the whole too large and too capriciously distributed to justify the use of the theory in this simplest form for other than approximate estimates or for comparative purposes. The airfoils were tested in two different wind tunnels and in one of the tunnels at two different air velocities, and the propeller characteristics computed from the three sets of airfoil data differ by as much as 28%, illustrating quite forcibly the necessity for having the airfoil tests made at the correct scale.
In spite of all its inaccuracies the simple blade-element theory has been a useful tool in the hands of experienced propeller designers. With it a skilful designer having a knowledge of suitable empirical factors can design propellers which usually fit the main conditions imposed upon them fairly well in that they absorb the engine power at very nearly the proper revolution speed. They are not, however, necessarily the most efficient propellers for their purpose, for the simple theory is not sufficiently accurate to show slight differences in efficiency due to changes in pitch distribution, plan forms, etc.
= Example
=In choosing a propeller to analyze, it is desirable that its aerodynamic characteristics be known so that the accuracy of the calculated results can be checked. It is also desirable that the analysis be made of a propeller operating at a relatively low tip speed in order to be free from any effects of compressibility and that it be running free from body interference. The only propeller tests which satisfy all of these conditions are tests of model propellers in a wind tunnel. We shall therefore take for our example the central or master propeller of a series of model wood propellers of standard Navy form, tested by Dr. W. F. Durand at Stanford University. This is a two-bladed propeller 3 ft. in diameter, with a uniform geometrical pitch of 2.1 ft. (or a pitch-diameter ratio of 0.7). The blades have standard propeller sections based on the R.A.F-6 airfoil (Fig. 6), and the blade widths, thicknesses, and angles are as given in the first part of Table I. In our analysis we shall consider the propeller as advancing with a velocity of 40 m.p.h. and turning at the rate of 1,800 r.p.m.For the section at 75% of the tip radius, the radius is 1.125 ft., the blade width is 0.198 ft., the thickness ratio is 0.107, the lower camber is zero, and the blade angle β is 16.6°.
The forward velocity
V
=
40
m
.
p
.
h
.
=
40
×
88
60
=
58.65
ft./sec.
,
{\displaystyle {\begin{aligned}V&=40\ \mathrm {m.p.h.} \\&={\frac {40\times 88}{60}}\\&=58.65\ {\text{ft./sec.}},\end{aligned}}}
and
n
=
1800
60
=
30
r.p.s.
{\displaystyle {\begin{aligned}n&={\frac {1800}{60}}\\&=30\ {\text{r.p.s.}}\end{aligned}}}
The path angle
ϕ
=
arctan
V
2
π
r
n
=
arctan
58.65
2
π
×
1.125
×
30
=
15.5
∘
{\displaystyle {\begin{aligned}\phi &=\arctan {\frac {V}{2\pi rn}}\\&=\arctan {\frac {58.65}{2\pi \times 1.125\times 30}}\\&=15.5^{\circ }\end{aligned}}}
The angle of attack is therefore
α
=
β
−
ϕ
=
16.6
∘
−
15.5
∘
=
1.1
∘
{\displaystyle {\begin{aligned}\alpha &=\beta -\phi \\&=16.6^{\circ }-15.5^{\circ }\\&=1.1^{\circ }\\\end{aligned}}}
From Fig. 7, for a flat-faced section of thickness ratio 0.107 at an angle of attack of 1.1°, γ = 3.0°, and, from Fig. 9, CL = 0.425. (For sections having lower camber, CL should be corrected in accordance with the relation given in Fig. 8, and γ is given the same value as that for a flat-faced section having the upper camber only.)
Then
K
=
C
L
b
sin
2
ϕ
cos
γ
=
0.425
×
0.198
0.2672
2
×
0.999
=
1.180
,
{\displaystyle {\begin{aligned}K&={\frac {C_{L}b}{\sin ^{2}\phi \cos \gamma }}\\&={\frac {0.425\times 0.198}{0.2672^{2}\times 0.999}}\\&=1.180,\end{aligned}}}
and,
T
C
=
K
cos
(
ϕ
+
γ
)
=
1.180
×
cos
18.5
∘
=
1.119.
{\displaystyle {\begin{aligned}T_{C}&=K\cos(\phi +\gamma )\\&=1.180\times \cos 18.5^{\circ }\\&=1.119.\\\end{aligned}}}
Also,
Q
C
=
K
r
sin
(
ϕ
+
γ
)
=
1.180
×
1.125
×
sin
18.5
∘
=
1.421.
{\displaystyle {\begin{aligned}Q_{C}&=Kr\sin(\phi +\gamma )\\&=1.180\times 1.125\times \sin 18.5^{\circ }\\&=1.421.\end{aligned}}}
The computations of Tc and Qc for six representative elements of the propeller are given in convenient tabular form in Table I, and the values of Tc and Qc are plotted against radius in Fig. 9. The curves drawn through these points are sometimes referred to as the torque grading curves. The areas under the curve represent
∫
0
R
T
c
d
r
{\displaystyle \int _{0}^{R}T_{c}dr}
and
∫
0
R
Q
c
d
r
,
{\displaystyle \int _{0}^{R}Q_{c}dr,}
these being the expressions for the total thrust and torque per blade per unit of dynamic pressure due to the velocity of advance. The areas may be found by means of a planimeter, proper consideration, of course, being given to the scales of values, or the integration may be performed approximately (but with satisfactory accuracy) by means of Simpson's rule.
In using Simpson's rule the radius is divided into an even number of equal parts, such as ten. The ordinate at each division can then be found from the grading curve. If the original blade elements divide the blade into an even number of equal parts it is not necessary to plot the grading curves, but the curves are advantageous in that they show graphically the distribution of thrust and torque along the blade. They also provide a check upon the computations, for incorrect points will not usually form a fair curve.
If the abscissas are denoted by r and the ordinates at the various divisions by y1, y2, ..., y11, according to Simpson’s rule the area with ten equal divisions will be
∫
0
R
F
(
r
)
d
r
=
Δ
r
3
[
y
1
+
2
(
y
3
+
y
5
+
y
7
+
y
9
)
+
4
(
y
2
+
y
4
+
y
6
+
y
8
+
y
10
)
+
y
11
]
.
{\displaystyle \int _{0}^{R}F(r)\,dr={\frac {\Delta r}{3}}[y_{1}+2(y_{3}+y_{5}+y_{7}+y_{9})+4(y_{2}+y_{4}+y_{6}+y_{8}+y_{10})+y_{11}].}
The area under the thrust-grading curve of our example is therefore
∫
0
R
T
c
d
r
=
0.15
3
[
0
+
2
(
0.038
+
0.600
+
1.050
+
1.091
)
+
4
(
0
+
0.253
+
0.863
+
1.120
+
0912
)
+
0
]
=
0.9075
,
{\displaystyle {\begin{aligned}\int _{0}^{R}T_{c}dr&={\frac {0.15}{3}}[0+2(0.038+0.600+1.050+1.091)+4(0+0.253+0.863+1.120+0912)+0]\\&=0.9075,\end{aligned}}}
and in like manner
∫
0
R
Q
c
d
r
=
0.340.
{\displaystyle \int _{0}^{R}Q_{c}\,dr=0.340.}
The above integrations have also been made by means of a planimeter, and the average results from five trials agree with those obtained by means of Simpson’s rule within one-fourth of one per cent.
The thrust of the propeller in standard air is
T
=
1
2
ρ
V
2
B
∫
0
R
T
c
d
r
=
1
2
×
0.002378
×
58.65
2
×
2
×
0.9075
=
7.42
l
b
.
,
{\displaystyle {\begin{aligned}T&={\frac {1}{2}}\rho V^{2}B\int _{0}^{R}T_{c}dr\\&={\frac {1}{2}}\times 0.002378\times 58.65^{2}\times 2\times 0.9075\\&=7.42\ \mathrm {lb.} ,\end{aligned}}}
and the torque is
Q
=
1
2
ρ
V
2
B
∫
0
R
Q
c
d
r
=
1
2
×
0.002378
×
58.65
2
×
2
×
0.340
=
2.78
l
b
.
f
t
.
{\displaystyle {\begin{aligned}Q&={\frac {1}{2}}\rho V^{2}B\int _{0}^{R}Q_{c}dr\\&={\frac {1}{2}}\times 0.002378\times 58.65^{2}\times 2\times 0.340\\&=2.78\ \mathrm {lb.ft.} \end{aligned}}}
The power absorbed by the propeller is
P
=
2
π
n
Q
=
2
×
π
×
30
×
2.78
=
524
f
t
.
l
b
.
/
s
e
c
.
{\displaystyle {\begin{aligned}P&=2\pi nQ\\&=2\times \pi \times 30\times 2.78\\&=524\ \mathrm {ft.lb./\ sec} .\end{aligned}}}
or
H
P
=
524
550
=
0.953
,
{\displaystyle {\begin{aligned}HP&={\frac {524}{550}}\\&=0.953,\end{aligned}}}
and the efficiency is
η
=
T
V
2
π
n
Q
=
7.42
×
58.65
524
=
0.830.
{\displaystyle {\begin{aligned}\eta &={\frac {TV}{2\pi nQ}}\\&={\frac {7.42\times 58.65}{524}}\\&=0.830.\end{aligned}}}
The above-calculated performance compares with that measured in the wind tunnel as follows:
The power as calculated by the simple blade-element theory is in this case over 11% too low, the thrust is about 5 % low, and the efficiency is about 8% high. Of course, a differently calculated performance would have been obtained if propeller-section characteristics from tests on the same series of airfoils in a different wind tunnel had been used, but the variable-density tunnel tests are probably the most reliable of all.
Some light may be thrown upon the discrepancy between the calculated and observed performance by referring again to the pressure distribution tests on a model propeller. In these tests the pressure distribution over several sections of a propeller blade was measured while the propeller was running in a wind tunnel, and the three following sets of tests were made on corresponding airfoils:
The results of these three sets of airfoil tests are shown for the section at three-fourths of the tip radius in Fig. 10, which has been taken from the report. It will be noticed that the coefficients of resultant force CR agree quite well for the median section of the airfoil of aspect ratio 6 and the corresponding section of the special propeller-blade airfoil but that the resultant force coefficient for the entire airfoil of aspect ratio 6 is considerably lower. It is natural, then, that the calculated thrust and power of a propeller should be too low when based on airfoil characteristics for aspect ratio 6.
Modifications
Many modifications to the simple blade-element theory have been suggested in order to make it more complete and to improve its accuracy. Most of these modified theories attempt to take into account the blade interference, and, in some of them, attempts are also made to eliminate the inaccuracy due to the use of airfoil data from tests on wings having a finite aspect ratio, such as 6. The first modification to be made was in the nature of a combination of the simple Drzewiecki theory with the Froude momentum theory.
Diagrams
Standard propeller sections based of R.A.F.-6 Infinite aspect ratio.
Attribution
This article incorporates text from this source, which is in the public domain: Weick, Fred Ernest (1899). Aircraft propeller design. New York, McGraw-Hill Book Company, inc.
See also
Circulation (fluid dynamics)
Computational fluid dynamics
External links
Blade Element Analysis for Propellers
Helicopter Theory - Blade Element Theory in Forward Flight from Aerospaceweb.org
Blade element theory
Stefan Drzewiecki 1903
QBlade: Open Source Blade Element Method Software from H.F.I. TU Berlin
NASA-TM-102219: A survey of nonuniform inflow models for rotorcraft flight dynamics and control applications, by Robert Chen, NASA
References
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- Blade element theory
- Blade element momentum theory
- Axial fan design
- Propeller theory
- William Froude
- Stefan Drzewiecki
- Momentum theory
- Wind-turbine aerodynamics
- Bet
- Propeller (aeronautics)
