In numerical mathematics, interval propagation or interval constraint propagation is the problem of contracting interval domains associated to variables of R without removing any value that is consistent with a set of constraints (i.e., equations or inequalities). It can be used to propagate uncertainties in the situation where errors are represented by intervals.[1] Interval propagation considers an estimation problem as a constraint satisfaction problem.
A contractor associated to an equation involving the variables x1,...,xn is an operator which contracts the intervals [''x''<sub>1</sub>],..., [''x''<sub>''n''</sub>] (that are supposed to enclose the xi's) without removing any value for the variables that is consistent with the equation.
A contractor is said to be atomic if it is not built as a composition of other contractors. The main theory that is used to build atomic contractors are based on interval analysis.
Example. Consider for instance the equation
x1+x2=x3,
which involves the three variables x1,x2 and x3.
The associated contractor is given by the following statements
[x3]:=[x3]\cap([x1]+[x2])
[x1]:=[x1]\cap([x3]-[x2])
[x2]:=[x2]\cap([x3]-[x1])
For instance, if
x1\in[-infty,5],
x2\in[-infty,4],
x3\in[6,infty]
the contractor performs the following calculus
x3=x1+x2 ⇒ x3\in[6,infty]\cap([-infty,5]+[-infty,4])=[6,infty]\cap[-infty,9]=[6,9].
x1=x3-x2 ⇒ x1\in[-infty,5]\cap([6,infty]-[-infty,4])=[-infty,5]\cap[2,infty]=[2,5].
x2=x3-x1 ⇒ x2\in[-infty,4]\cap([6,infty]-[-infty,5])=[-infty,4]\cap[1,infty]=[1,4].
For other constraints, a specific algorithm for implementing the atomic contractor should be written. An illustration is the atomic contractor associated to the equation
x2=\sin(x1),
is provided by Figures 1 and 2.
For more complex constraints, a decomposition into atomic constraints (i.e., constraints for which an atomic contractor exists) should be performed. Consider for instance the constraint
x+\sin(xy)\leq0,
could be decomposed into
a=xy
b=\sin(a)
c=x+b.
The interval domains that should be associated to the new intermediate variables are
a\in[-infty,infty],
b\in[-1,1],
c\in[-infty,0].
The principle of the interval propagation is to call all available atomic contractors until no more contraction could be observed. [2] As a result of the Knaster-Tarski theorem, the procedure always converges to intervals which enclose all feasible values for the variables. A formalization of the interval propagation can be made thanks to the contractor algebra. Interval propagation converges quickly to the result and can deal with problems involving several hundred of variables.[3]
Consider the electronic circuit of Figure 3. Assume that from different measurements, we know that
E\in[23V,26V]
I\in[4A,8A]
U1\in[10V,11V]
U2\in[14V,17V]
P\in[124W,130W]
R1\in[0\Omega,infty]
R2\in[0\Omega,infty].
From the circuit, we have the following equations
P=EI
U1=R1I
U2=R2I
E=U1+U2.
After performing the interval propagation, we get
E\in[24V,26V]
I\in[4.769A,5.417A]
U1\in[10V,11V]
U2\in[14V,16V]
P\in[124W,130W]
R1\in[1.846\Omega,2.307\Omega]
R2\in[2.584\Omega,3.355\Omega].