advanced21 min studyLesson 382 in Mathematics

Sobolev norms and completeness

Measure functions and weak derivatives together, and prove that limits preserve the derivative identities.

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What you’ll understand

  • Compute a full Sobolev norm and distinguish it from a derivative seminorm.
  • Prove completeness by passing weak derivative identities to Lᵖ limits.
  • Identify the Hilbert structure of Hᵏ and the meaning of the zero-boundary closure.

A derivative estimate alone does not record the size of the function: adding a large constant leaves the gradient unchanged. Sobolev norms solve this by measuring the function and its weak derivatives in the same integrability scale. Their completeness is what allows approximation sequences, numerical trial functions, and energy-minimizing sequences to converge inside a mathematically stable space. The essential proof checks that the limit of the proposed derivatives really differentiates the limit function.

The full norm includes order zero

For an open set Ω\Omega, an integer k≥0k\ge0, and 1≤p≤∞1\le p\le\infty, the space Wk,p(Ω)W^{k,p}(\Omega) consists of LpL^p equivalence classes whose weak derivatives through order kk also belong to LpL^p. For finite pp, use the pth root of the sum of all derivative pth powers, including D0u=uD^0u=u. For p=∞p=\infty, take the maximum of the finitely many essential-supremum derivative norms. Other finite sums define equivalent norms, but a numerical norm calculation must state its convention.

By the highest-order seminorm, we mean ∣u∣Wk,p=(∑∣α∣=k∥Dαu∥pp)1/p|u|_{W^{k,p}}=(\sum_{|\alpha|=k}\|D^\alpha u\|_p^p)^{1/p} for finite p and positive k, using only derivatives of exactly order k. For k equal to one it is the gradient seminorm, with constants in its kernel on each connected component. For higher orders, polynomials of lower degree also lie in this highest-order kernel whenever they belong to the underlying LpL^p space. Boundary or mean restrictions can remove this kernel, leading later to Poincaré inequalities. Domain size also affects scaling: rescaling a coordinate changes the sizes of a function and its derivative by different powers. Dimensionally scaled norms are sometimes convenient in finite-element analysis, but they must not be silently substituted into an unscaled energy computation.

∥u∥Wk,p(Ω)=(∑∣α∣≤k∥Dαu∥Lp(Ω)p)1/p(1≤p<∞)\|u\|_{W^{k,p}(\Omega)}=\left(\sum_{|\alpha|\le k}\|D^\alpha u\|_{L^p(\Omega)}^p\right)^{1/p}\quad(1\le p<\infty)
The order-zero term is essential: it prevents nonzero constants from having zero norm.↔ Scroll wide equations horizontally.

Why the derivative graph is closed

Take a Cauchy sequence in this full norm. Completeness of LpL^p supplies a limit uu for the functions and a limit gαg_\alpha for each derivative component. For every compactly supported test, Hölder's inequality lets us pass the weak identity to the limit, since the test and its derivatives belong to the appropriate conjugate spaces on their compact support. Consequently gα=Dαug_\alpha=D^\alpha u as a distribution, and it is represented by an LpL^p function. The limits are compatible because the derivative relation is closed, not because arbitrary independent limits automatically match.

There are only finitely many derivative components up to the fixed order, so componentwise convergence implies convergence in the Sobolev norm. This proves that Wk,pW^{k,p} is Banach, including the endpoint cases one and infinity. For 1<p<∞1<p<\infty, finite products of LpL^p spaces are reflexive, and the closed derivative graph inherits reflexivity. This additional property often supplies weakly convergent subsequences from bounded families. It is separate from completeness: a complete space need not make every bounded sequence strongly convergent, or even weakly sequentially compact at the endpoint exponents.

uj→u,Dαuj→gα in Lp ⟹ ∫ΩuDαφ=(−1)∣α∣∫Ωgαφu_j\to u,\quad D^\alpha u_j\to g_\alpha\text{ in }L^p\ \Longrightarrow\ \int_\Omega uD^\alpha\varphi=(-1)^{|\alpha|}\int_\Omega g_\alpha\varphi
Passing the distributional identity to the limit identifies each derivative limit and proves the closed-graph step in completeness.↔ Scroll wide equations horizontally.

Hilbert energy and closed subspaces

The notation HkH^k means Wk,2W^{k,2}. Its norm comes from summing the L2L^2 inner products of matching derivative components, with complex conjugation in the complex-valued setting. Orthogonal projection and Hilbert-space methods can therefore be applied to approximation problems. A minimizing sequence need not converge strongly just because it is bounded; one often first obtains weak convergence and then uses lower semicontinuity. Knowing which topology a compactness argument produces prevents an unjustified passage through nonlinear expressions.

For finite pp, define W01,p(Ω)W^{1,p}_0(\Omega) as the closure of Cc∞(Ω)C_c^\infty(\Omega) in the full first-order Sobolev norm. It is complete because it is a closed subspace. The subscript zero is not a statement about assigning zeros to arbitrary pointwise boundary representatives. On bounded Lipschitz domains it agrees with the kernel of the trace map, a theorem developed later. On the whole space, compactly supported smooth functions are dense for finite pp, while on a bounded domain they cannot approximate a function with nonzero trace in the same norm.

Compute a complete energy norm

With the unscaled norm ∥u∥H12=∫01(∣u∣2+∣u′∣2)\|u\|_{H^1}^2=\int_0^1(|u|^2+|u'|^2), compute the norm of u(x)=x(1−x)u(x)=x(1-x) and explain why its gradient seminorm differs.

  1. Differentiate to obtain u′=1−2xu'=1-2x. The function and derivative are square integrable, so the classical derivative is also its weak derivative and u∈H1(0,1)u\in H^1(0,1).

  2. Expand the square of the function: ∫01(x2−2x3+x4)=1/3−1/2+1/5=1/30\int_0^1(x^2-2x^3+x^4)=1/3-1/2+1/5=1/30. For the derivative, ∫01(1−2x)2=1−2+4/3=1/3\int_0^1(1-2x)^2=1-2+4/3=1/3.

  3. Add the order-zero and derivative terms: ∥u∥H12=11/30\|u\|_{H^1}^2=11/30. Its gradient seminorm is only 1/31/\sqrt3, whereas the full norm is 11/30\sqrt{11/30}.

The result

The full norm records both mass and variation. Omitting the function term changes this calculation and loses control of constants on unrestricted H¹.

Explore the model

Interactive lab

Interactive lab · heat

Equal mass does not mean equal derivative energy

Pause and Reset; set mode n to 1 and diffusivity κ to 0.5. At time zero its L² readout is π\sqrt\pi. Reset and set n to 3 and κ to 0.5: predict the same L² value but a three-times-larger derivative L² norm, computed on paper as nπn\sqrt\pi. Step to compare their decay.

Equal mass does not mean equal derivative energyThe exact periodic heat-equation mode is u(x,t) = exp(−κn²t) sin(nx), on [0,2π]. Playback advances physical time. The initial sine is shown separately, and the unnormalized L² norm is √π exp(−κn²t). This analytic instrument does not run a finite-difference solver or test discretization stability. Current readings: Current amplitude: 1; Spatial L² norm: 1.772; Decay rate · κn²: 3.6 /s. All parameters are adjustable with the labeled controls below.Periodic heat equation mode 3 at time 0: the amplitude is 1.0π/2π3π/22π−1−0.500.51x · periodic intervalTemperature perturbation uExact mode · n = 3
Current temperature modeInitial sineCurrent amplitude
Current amplitude
1
Spatial L² norm
1.772
Decay rate · κn²
3.6 /s
t = 0 s

The exact periodic heat-equation mode is u(x,t) = exp(−κn²t) sin(nx), on [0,2π]. Playback advances physical time. The initial sine is shown separately, and the unnormalized L² norm is √π exp(−κn²t). This analytic instrument does not run a finite-difference solver or test discretization stability. Parameter changes pause playback and recompute the model at the current elapsed time. Reset restores both parameters and returns time to zero. Playback starts paused. Adjust either parameter, then choose Play or Step.

Look forThe exact periodic sine model shows that derivative energy weights higher frequencies more heavily. Its displayed L² norm is not a full H¹ norm; the derivative term must be calculated separately.

Check your understanding

Why does the gradient L² quantity fail to be a norm on unrestricted H¹(0,1)?

Try it yourself

Let uj(x)=x2+x/ju_j(x)=x^2+x/j on (0,1)(0,1). Prove convergence in the same H¹ norm to u=x2u=x^2, and compute ∥u∥H12\|u\|_{H^1}^2.

Take a moment to make a prediction or work it out on paper. Open a hint when you need one.

Give me a hint

Compute the function difference and its derivative before integrating their squares.

Compare with the solution

The difference is x/jx/j with derivative 1/j1/j. Its squared H¹ norm is (1/j2)(1/3+1)=4/(3j2)(1/j^2)(1/3+1)=4/(3j^2), which tends to zero. For the limit, ∫01x4=1/5\int_0^1x^4=1/5 and ∫01(2x)2=4/3\int_0^1(2x)^2=4/3, so ∥x2∥H12=23/15\|x^2\|_{H^1}^2=23/15. Both function and derivative converge in their required L² components.

Take it with you

  • A full Sobolev norm includes the function itself as well as derivatives.
  • Completeness relies on closed distributional derivative identities.
  • Reflexivity, strong compactness, and Hilbert structure are additional properties with their own hypotheses.

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