The actual normalized pressure in the transverse forward equation #
The scalar L² primitive and the literal periodic integral are identified. Its angular derivative closes equation (11) for the constructed physical field. The pressure is smooth in the cylinder variables, has zero angular mean, and retains the same spatial support.
Genuine mixed regularity of the solved physical forward fields #
The actual coordinate solve and its ordinary right side have smooth mixed translation orbits. Applying the physical frame then gives this same regularity for the velocity and its true time derivative. These statements are proved from the data, not included in the solution interface.
Actual unnormalized forward solutions have smooth mixed translation orbits.
The constructed unnormalized path is genuinely smooth in all covering parameters. This qualitative statement needs no propagator bound or smoothness of a time profile.
The actual pointwise forward equation #
The L² coordinate equation and normal balance hold for the reconstructed smooth field at every cylinder point. The scalar normal residual is the literal source expression; its angular primitive will supply the pressure.
The solved forward field as an actual smooth cylinder field #
The representative is recovered by bounded H3 evaluation of the genuine L² solution. It is jointly continuous, spatially and angularly smooth, compactly supported, and has the true pointwise within-time derivative.
The actual physical field, reconstructed from the solved L² class.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The reconstructed actual product-rule time derivative.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Inclusion in full cylinder L² preserves the already proved time derivative.
No global time extension is assumed: the true time derivative holds within the closed source interval, at every cylinder point.
The source's literal scalar normal pressure residual.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The literal scalar pressure source is smooth in every spatial and angular variable.
Pointwise tangency follows from the actual frame representation and continuity.
Equation (11) before angular integration holds at every cylinder point.
The solved normal pressure source has zero angular mean #
The zero mode is proved for the actual Duhamel solution and then transferred to its continuous scalar representative. No zero-mean condition on the solution or on its pressure residual is assumed.
The actual scalar pressure source on cylinder L² #
The normal functional is constructed from the positive one-column Gram matrix. Applying it to f−2MA gives a genuine scalar L² path, with the literal normal residual as representative and genuine smooth mixed translation orbit.
A genuine supported scalar path representing the right side of ∂θπ in (11).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The pressure source is precisely the manuscript's scalar quotient.
The actual scalar pressure source inherits genuine mixed regularity from the solve.
The actual scalar L² class represents the literal normal quotient.
Zero mean of the forcing and initial coordinate implies zero mean of the literal pressure source of the constructed solution.
The actual bounded angular inverse applied to the solved scalar source.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The literal normalized periodic pressure for the actual forward solution.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The derivative is genuine at every real angle, including period endpoints.
Equation (11) with the actual angular derivative of the normalized pressure.