Orthogonality of Two Functions

Click For Summary
SUMMARY

The discussion focuses on proving the orthogonality of two functions, specifically \varphi_{0}(x) = f_{0}(x) and \varphi_{1}(x) = f_{1}(x) - \frac{\left\langle\right\varphi_{0},f_{1}\rangle}{\left\|\varphi_{0}\right\|^{2}}\varphi_{0}(x), over the interval [a,b]. The key to the proof lies in demonstrating that the inner product \left\langle\right\varphi_{0},\varphi_{1}\rangle equals zero, which is established through integration. The discussion emphasizes the use of the Delta Kronecker property, where \delta_{mn} is zero for m and n not equal, simplifying the proof process.

PREREQUISITES
  • Understanding of inner product spaces and orthogonality in functional analysis.
  • Familiarity with the Delta Kronecker notation and its implications in proofs.
  • Knowledge of integration techniques, particularly integration by parts.
  • Proficiency in handling definite integrals and their properties.
NEXT STEPS
  • Study the properties of inner products in functional spaces.
  • Learn about the application of the Delta Kronecker in orthogonality proofs.
  • Explore integration by parts and its applications in solving complex integrals.
  • Investigate the implications of orthogonal functions in various mathematical contexts.
USEFUL FOR

Students and professionals in mathematics, particularly those studying functional analysis, as well as educators looking to enhance their understanding of orthogonality and integration techniques.

White Ink
Messages
18
Reaction score
0

Homework Statement



Show that:

[tex]\varphi_{0}(x) = f_{0}(x)[/tex]

and

[tex]\varphi_{1}(x) = f_{1}(x) - \frac{\left\langle\right\varphi_{0},f_{1}\rangle}{\left\|\varphi_{0}\right\|^{2}}\varphi_{0}(x)[/tex]

are orthogonal on the interval [a,b].

Homework Equations



Orthogonal functions satisfy:

[tex]\left\langle\right\varphi_{m},\varphi_{n}\rangle = \int^{b}_{a}\varphi_{m}(x)\varphi_{n}(x)dx = g(m)\delta_{mn}[/tex]

Where, [tex]\delta_{mn}[/tex] is the Delta Kronecker.

Also:

[tex]\left\langle\right\varphi_{m},\varphi_{m}\rangle = \left\|\varphi_{m}\right\|^{2}[/tex]

The Attempt at a Solution



Since m and n (0 and 1) are not equal, the Delta Kronecker is zero and therefore the proof is a matter of proving that:

[tex]\left\langle\right\varphi_{0},\varphi_{1}\rangle = 0[/tex]

Having substituted the functions into the inner product formula in 2:

[tex]\left\langle\right\varphi_{0},\varphi_{1}\rangle = \int^{b}_{a}\varphi_{0}(x)\varphi_{1}(x)dx = <br /> \int^{b}_{a}f_{0}(x)\left[f_{1}(x) - \frac{\left\langle\right\varphi_{0},f_{1}\rangle}{\left\|\varphi_{0}\right\|^{2}}\varphi_{0}(x)\right]dx[/tex]

Because the Delta Kronecker is zero, all I have to do is show that:

[tex]\int^{b}_{a}f_{0}(x)\left[f_{1}(x) - \frac{\left\langle\right\varphi_{0},f_{1}\rangle}{\left\|\varphi_{0}\right\|^{2}}\varphi_{0}(x)\right]dx = 0[/tex]

I'm unsure as to whether I should use integration by parts to do the resulting integral because there is another integral embedded in the [tex]\varphi_{1}(x)[/tex] function; which (because it is a definite integral) would be tricky to differentiate or integrate.
 
Physics news on Phys.org
You really don't need to bring the Kronecker delta stuff into the picture. It is completely superfluous. You do need to show that [itex]\langle \varphi_0, \varphi_1 \rangle = 0[/itex] as that is the definition of orthogonality.

Why integrate by parts? Use [itex]\langle f, g \rangle \equiv \int_a^b f(x)g(x)\,dx[/itex] and [itex]\varphi_0(x) = f_0(x)[/itex]
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 9 ·
Replies
9
Views
2K
Replies
20
Views
2K
  • · Replies 12 ·
Replies
12
Views
3K
Replies
16
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 105 ·
4
Replies
105
Views
11K