
The section lift coefficient is related to the section lift by:
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So that if we know the lift distribution and the planform shape, we can
find the Cl distribution.
The lift and lift coefficient distributions are directly related by the
chord distribution. Here are some examples:

The lift and Cl distributions can be divided into so-called basic and additional
lift distributions. This division allows one to examine the lift distributions
at a couple of angles of attack and to infer the lift distribution at all
other angles. This is especially useful in the process of wing design.
From the discussion of lifting line theory and Weissinger theory,
we saw that the distribution of lift could be written:
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where:
αr is the angle of attack at the root
θ is the twist angle
{l1} is the wing lift distribution with no twist and with αr = 1
{l2} is the lift distribution at zero angle of attack and unit twist.
The lift distribution may also be written in a more conventional way:
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Here, the distributions {la} and {lb} are the wing lift distributions with
no twist at CL = 1 and with unit twist at zero lift respectively. The first
term, CL {la}, is called the additional lift. It is the lift distribution
that is added by increasing the total wing lift. θ {lb} is called
the basic lift distribution and is the lift distribution at zero lift.
Why is this useful? Consider the following example.

We can use the data at these two angles of attack to learn a great deal about the wing.
From the expression above:
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or:
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The additional lift distribution, CL {la} may be interpreted graphically
as shown below.

The additional lift coefficient distribution at CL = 1.0 is plotted below.
Note that it rises upward
toward the tip -- this is indicative of a wing with a very low taper ratio
or a wing with sweep-back.

The basic lift distribution is negative near the tip implying that the wing
has washout.