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Graduate · Fourier incompressibility projection · 89 of 650

Fourier incompressibility projection · Frequency component k₁=1.5; Frequency component k₂=2.5

Use θ=6π/5 radians. Compute the projected coefficient Pₖv=v−k(k·v)/|k|², its dot product with k, and its norm. Givens: Frequency component k₁=1.5; Frequency component k₂=2.5.

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01 · Make a prediction

Your practice question

At the nonzero Fourier frequency k=(1.5,2.5), use the real unit coefficient v=(cos θ,sin θ). Use θ=6π/5 radians. Compute the projected coefficient Pₖv=v−k(k·v)/|k|², its dot product with k, and its norm.

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02 · Explore the model

See the mathematical relationship move.

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Watch the relationship

Paused
Fourier incompressibility projection · Frequency component k₁=1.5; Frequency component k₂=2.5. Projected x: 0.735. Projected y: -0.441. k dot projected vector: 0. Projected norm: 0.857Remove the longitudinal componentxy0InputProjectionResidualEqual axis scales · coordinates in the readouts
This is one real two-dimensional Fourier coefficient and a nonzero frequency, not a complete velocity field. The algebraic projection is exact. Boundary conditions and pressure reconstruction for a global fluid problem are outside this scene.

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Make it your experiment

Change one value. Notice what follows.

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Projected x
0.735
Projected y
-0.441
k dot projected vector
0
Projected norm
0.857

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The mathematical idea

At a nonzero Fourier frequency, incompressibility requires the velocity coefficient to be perpendicular to that frequency. The orthogonal projection removes only the longitudinal component. Rotating an input coefficient shows which information is kept and which is discarded without pretending to solve the full fluid dynamics. At the nonzero Fourier frequency k=(1.5,2.5), use the real unit coefficient v=(cos θ,sin θ). Use θ=6π/5 radians. The requested state occurs at 60% playback; use the exact target stated in the question for your calculation.

Pₖv=v−k(k·v)/|k|²; k·Pₖv=0

03 · Reflect and transfer

Explain what changes and why.

Why does projecting this one Fourier coefficient neither evolve the whole velocity field nor settle the general Navier–Stokes regularity problem?

This is a distinct guided scenario using a reusable mathematical model. Similar-looking diagrams can represent different given values and conclusions; they are not different mathematical theories.