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# Tutorial: Building a Reduced Basis¶

In this tutorial we will learn more about VectorArrays and how to construct a reduced basis using pyMOR.

A reduced basis spans a low dimensional subspace of a Model’s solution_space, in which the solutions of the Model can be well approximated for all parameter values. In this context, time is treated as an additional parameter. So for time-dependent problems, the reduced space (the span of the reduced basis) should approximate the solution for all parameter values and time instances.

An upper bound for the possible quality of a reduced space is given by the so-called Kolmogorov $$N$$-width $$d_N$$ given as

$\begin{split}d_N := \inf_{\substack{V_N \subseteq V\\ \operatorname{dim}(V_N) \leq N}}\, \sup_{\mu \in \mathcal{P}}\, \inf_{v \in V_N}\, \|u(\mu) - v\|.\end{split}$

In this formula $$V$$ denotes the solution_space, $$\mathcal{P} \subset \mathbb{R}^p$$ denotes the set of all parameter values we are interested in, and $$u(\mu)$$ denotes the solution of the Model for the given parameter values $$\mu$$. In pyMOR the set $$\mathcal{P}$$ is called the ParameterSpace.

How to read this formula? For each candidate reduced space $$V_N$$ we look at all possible parameter values $$\mu$$ and compute the best-approximation error in $$V_N$$ (the second infimum). The supremum over the infimum is thus the worst-case best-approximation error over all parameter values of interest. Now we take the infimum of the worst-case best-approximation errors over all possible reduced spaces of dimension at most $$N$$, and this is $$d_N$$.

So whatever reduced space of dimension $$N$$ we pick, we will always find a $$\mu$$ for which the best-approximation error in our space is at least $$d_N$$. Reduced basis methods aim at constructing spaces $$V_N$$ for which the worst-case best-approximation error is as close to $$d_N$$ as possible.

However, we will only find a good $$V_N$$ of small dimension $$N$$ if the values $$d_N$$ decrease quickly for growing $$N$$. It can be shown that this is the case as soon as $$u(\mu)$$ analytically depends on $$\mu$$, which is true for many problems of interest. More precisely, it can be shown [BCD+11], [RD13] that there are constants $$C, c > 0$$ such that

$d_N \leq C \cdot e^{-N^c}.$

In this tutorial we will construct reduced spaces $$V_N$$ for a concrete problem with pyMOR and study their error decay.

## Model setup¶

First we need to define a Model and a ParameterSpace for which we want to build a reduced basis. We choose here the standard thermal block benchmark problem shipped with pyMOR (see Getting started). However, any pyMOR Model can be used, except for Section Weak Greedy Algorithm where some more assumptions have to be made on the Model.

First we import everything we need:

import numpy as np
from pymor.basic import *


Then we build a 3-by-3 thermalblock problem that we discretize using pyMOR’s builtin discretizers (see Tutorial: Using pyMOR’s discretization toolkit for an introduction to pyMOR’s discretization toolkit).

problem = thermal_block_problem((3,3))
fom, _ = discretize_stationary_cg(problem, diameter=1/100)


Next, we need to define a ParameterSpace of parameter values for which the solutions of the full-order model fom should be approximated by the reduced basis. We do this by calling the space method of the |parameters| of fom:

parameter_space = fom.parameters.space(0.0001, 1.)


Here, 0.0001 and 1. are the common lower and upper bounds for the individual components of all |parameters| of fom. In our case fom expects a single parameter 'diffusion' of 9 values:

fom.parameters

Parameters({diffusion: 9})


If fom were to depend on multiple |parameters|, we could also call the space method with a dictionary of lower and upper bounds per parameter.

The main use of ParameterSpaces in pyMOR is that they allow to easily sample parameter values from their domain using the methods sample_uniformly and sample_randomly.

## Computing the snapshot data¶

Reduced basis methods are snapshot-based, which means that they build the reduced space as a linear subspace of the linear span of solutions of the fom for certain parameter values. The easiest approach is to just pick these values randomly, what we will do in the following. First we define a training set of 25 parameters:

training_set = parameter_space.sample_randomly(25)
print(training_set)

[Mu({'diffusion': array([0.37460266, 0.95071923, 0.73202074, 0.59869862, 0.15610304,
0.15607892, 0.0581778 , 0.86618953, 0.6011549 ])}), Mu({'diffusion': array([0.70810177, 0.02068244, 0.96991286, 0.8324594 , 0.21241788,
0.18190678, 0.18348617, 0.30431182, 0.52480396])}), Mu({'diffusion': array([0.43200182, 0.29130002, 0.61189171, 0.13957991, 0.29221543,
0.36642521, 0.45612438, 0.78519744, 0.19975381])}), Mu({'diffusion': array([0.51428301, 0.59245533, 0.04654577, 0.6075841 , 0.17060707,
0.06514509, 0.94889065, 0.96563547, 0.80841651])}), Mu({'diffusion': array([0.30468331, 0.09776235, 0.6842646 , 0.44020848, 0.12212603,
0.49522739, 0.03448508, 0.90932947, 0.2588541 ])}), Mu({'diffusion': array([0.66255603, 0.3117799 , 0.52011601, 0.54675561, 0.18493597,
0.96958767, 0.77515531, 0.93950499, 0.89483787])}), Mu({'diffusion': array([0.59794019, 0.92188205, 0.08858365, 0.19606326, 0.04532277,
0.3253978 , 0.38873842, 0.2714219 , 0.82875464])}), Mu({'diffusion': array([0.35681765, 0.28100642, 0.54274181, 0.14101013, 0.80221676,
0.07464319, 0.98688825, 0.77226754, 0.19879581])}), Mu({'diffusion': array([0.00562156, 0.81547988, 0.70688666, 0.72903427, 0.77129322,
0.07413725, 0.35852988, 0.11595747, 0.86311712])}), Mu({'diffusion': array([0.6233358 , 0.33096494, 0.06365199, 0.31105122, 0.3252508 ,
0.72963322, 0.63759372, 0.88722402, 0.4722677 ])}), Mu({'diffusion': array([0.11968229, 0.71327346, 0.76080897, 0.56132107, 0.77099008,
0.49384622, 0.52278056, 0.42759826, 0.02551658])}), Mu({'diffusion': array([0.10798064, 0.03152604, 0.63644677, 0.31442455, 0.50861983,
0.90757572, 0.2493673 , 0.41044188, 0.75557558])}), Mu({'diffusion': array([0.22887529, 0.07707221, 0.28982248, 0.16130517, 0.92970468,
0.80813957, 0.63344042, 0.87147344, 0.80369171])}), Mu({'diffusion': array([0.1866514 , 0.89256974, 0.53938831, 0.80745941, 0.89610169,
0.31807167, 0.11014092, 0.22801237, 0.42716508])}), Mu({'diffusion': array([0.81803296, 0.86074451, 0.00705144, 0.51079623, 0.41746926,
0.2221856 , 0.11995338, 0.33768141, 0.94291541])}), Mu({'diffusion': array([0.32327061, 0.51883874, 0.70304866, 0.36369324, 0.9717849 ,
0.96245105, 0.25185712, 0.49729878, 0.30094822])}), Mu({'diffusion': array([0.28491201, 0.03698326, 0.60960338, 0.50272876, 0.0515736 ,
0.2787186 , 0.90827506, 0.23963793, 0.14498038])}), Mu({'diffusion': array([0.48950382, 0.98565189, 0.24213107, 0.67216833, 0.76164345,
0.23771378, 0.72824353, 0.36784635, 0.6323426 ])}), Mu({'diffusion': array([0.63356636, 0.53582111, 0.09038074, 0.83531897, 0.32084799,
0.18659986, 0.04087106, 0.59093385, 0.67759661])}), Mu({'diffusion': array([0.01668617, 0.51214185, 0.22657313, 0.64520827, 0.17444899,
0.69096864, 0.38679667, 0.93673632, 0.13760719])}), Mu({'diffusion': array([0.34113224, 0.11356217, 0.92470115, 0.87735162, 0.25801583,
0.66001805, 0.81724048, 0.55524529, 0.52969761])}), Mu({'diffusion': array([0.24192811, 0.09319346, 0.89722604, 0.90042802, 0.63313815,
0.33909589, 0.34927465, 0.72598308, 0.89712055])}), Mu({'diffusion': array([0.88709772, 0.77989756, 0.64206744, 0.08423155, 0.16171255,
0.89856433, 0.60646842, 0.00929613, 0.1015614 ])}), Mu({'diffusion': array([0.66353542, 0.00516108, 0.16089197, 0.54877892, 0.69192601,
0.65199606, 0.22434688, 0.712208  , 0.23732536])}), Mu({'diffusion': array([0.32546716, 0.74651676, 0.64966794, 0.84923849, 0.65764713,
0.56835177, 0.0937654 , 0.36777903, 0.26527585])})]


Then we solve the full-order model for all parameter values in the training set and accumulate all solution vectors in a single VectorArray using its append method. But first we need to create an empty VectorArray to which the solutions can be appended. New VectorArrays in pyMOR are always created by a corresponding VectorSpace. Empty arrays are created using the empty method. But what is the right VectorSpace? All solutions of a Model belong to its solution_space, so we write:

U = fom.solution_space.empty()
for mu in training_set:
U.append(fom.solve(mu))


Note that fom.solve returns a VectorArray containing a single vector. This entire array (of one vector) is then appended to the U array. pyMOR has no notion of single vectors, we only speak of VectorArrays.

What exactly is a VectorSpace? A VectorSpace in pyMOR holds all information necessary to build VectorArrays containing vector objects of a certain type. In our case we have

fom.solution_space

NumpyVectorSpace(20201, id='STATE')


which means that the created VectorArrays will internally hold NumPy arrays for data storage. The number is the dimension of the vector. We have here a NumpyVectorSpace because pyMOR’s builtin discretizations are built around the NumPy/SciPy stack. If fom would represent a Model living in an external PDE solver, we would have a different type of VectorSpace which, for instance, might hold a reference to a discrete functions space object inside the PDE solver instead of the dimension.

After appending all solutions vectors to U, we can verify that U now really contains 25 vectors:

len(U)

25


Note that appending one VectorArray V to another array U will append copies of the vectors in V to U. So modifying U will not affect V.

Let’s look at the solution snapshots we have just computed using the visualize method of fom. A VectorArray containing multiple vectors is visualized as a time series:

fom.visualize(U)


## A trivial reduced basis¶

Given some snapshot data, the easiest option to get a reduced basis is to just use the snapshot vectors as the basis:

trivial_basis = U.copy()


Note that assignment in Python never copies data! Thus, if we had written trivial_basis = U and modified trivial_basis, U would change as well, since trivial_basis and U would refer to the same VectorArray object. So whenever you want to use one VectorArray somewhere else and you are unsure whether some code might change the array, you should always create a copy. pyMOR uses copy-on-write semantics for copies of VectorArrays, which means that generally calling copy is cheap as it does not duplicate any data in memory. Only when you modify one of the arrays the data will be copied.

Now we want to know how good our reduced basis is. So we want to compute

$\inf_{v \in V_N}\ \|u(\mu) - v\|,$

where $$V_N$$ denotes the span of our reduced basis, for all $$\mu$$ in some validation set of parameter values. Assuming that we are in a Hilbert space, we can compute the infimum via orthogonal projection onto $$V_N$$: in that case, the projection will be the best approximation in $$V_N$$ and the norm of the difference between $$u(\mu)$$ and its orthogonal projection will be the best-approximation error.

So let $$v_{proj}$$ be the orthogonal projection of $$v$$ onto the linear space spanned by the basis vectors $$u_i,\ i=1, \ldots, N$$. By definition this means that $$v - v_{proj}$$ is orthogonal to all $$u_i$$:

$(v - v_{proj}, u_i) = 0, \qquad i = 1, \ldots, N.$

Let $$\lambda_j$$, $$j = 1, \ldots, N$$ be the coefficients of $$v_{proj}$$ with respect to this basis, i.e. $$\sum_{j=1}^N \lambda_j u_j = v_{proj}$$. Then:

$\sum_{j=1}^N \lambda_j (u_j, u_i) = (v, u_i), \qquad i = 1, \ldots, N.$

With $$G_{i,j} := (u_i, u_j)$$, $$R := [(v, u_1), \ldots, (v, u_N)]^T$$ and $$\Lambda := [\lambda_1, \ldots, \lambda_N]^T$$, we obtain the linear equation system

$G \cdot \Lambda = R,$

which determines $$\lambda_i$$ and, thus, $$v_{proj}$$.

Let’s assemble and solve this equation system using pyMOR to determine the best-approximation error in trivial_basis for some test vector V which we take as another random solution of our Model:

V = fom.solve(parameter_space.sample_randomly())


The matrix $$G$$ of all inner products between vectors in trivial_basis is a so called Gramian matrix. Consequently, every VectorArray has a gramian method, which computes precisely this matrix:

G = trivial_basis.gramian()


The Gramian is computed w.r.t. the Euclidean inner product. For the right-hand side $$R$$, we need to compute all (Euclidean) inner products between the vectors in trivial_basis and (the single vector in) V. For that, we can use the inner method:

R = trivial_basis.inner(V)


which will give us a $$25\times 1$$ NumPy array of all inner products.

Now, we can use NumPy to solve the linear equation system:

lambdas = np.linalg.solve(G, R)


Finally, we need to form the linear combination

$\sum_{j=1}^N \lambda_j u_j = v_{proj}$

using the lincomb method of trivial_basis. It expects row vectors of linear coefficients, but solve returns column vectors, so we need to take the transpose:

V_proj = trivial_basis.lincomb(lambdas.T)


Let’s look at V, V_proj and the difference of both. VectorArrays of the same length can simply be subtracted, yielding a new array of the differences:

# for some reason V_proj does not carry over from the previous cell
V_proj = trivial_basis.lincomb(lambdas.T)
fom.visualize((V, V_proj, V - V_proj),
legend=('V', 'V_proj', 'best-approximation err'),
separate_colorbars=True)


As you can see, we already have a quite good approximation of V with only 25 basis vectors.

Now, the Euclidean norm will just work fine in many cases. However, when the full-order model comes from a PDE, it will be usually not the norm we are interested in, and you may get poor results for problems with strongly anisotropic meshes.

For our diffusion problem with homogeneous Dirichlet boundaries, the Sobolev semi-norm (of order one) is a natural choice. Among other useful products, discretize_stationary_cg already assembled a corresponding inner product Operator for us, which is available as

fom.h1_0_semi_product

NumpyMatrixOperator(<20201x20201 sparse, 140601 nnz>, source_id='STATE', range_id='STATE', name='h1_0_semi')


Note

The 0 in h1_0_semi_product refers to the fact that rows and columns of Dirichlet boundary DOFs have been cleared in the matrix of the Operator to make it invertible. This is important for being able to compute Riesz representatives w.r.t. this inner product (required for a posteriori estimation of the ROM error). If you want to compute the H1 semi-norm of a function that does not vanish at the Dirichlet boundary, use fom.h1_semi_product.

To use fom.h1_0_semi_product as an inner product Operator for computing the projection error, we can simply pass it as the optional product argument to gramian and inner:

G = trivial_basis[:10].gramian(product=fom.h1_0_semi_product)
R = trivial_basis[:10].inner(V, product=fom.h1_0_semi_product)
lambdas = np.linalg.solve(G, R)
V_h1_proj = trivial_basis[:10].lincomb(lambdas.T)

fom.visualize((V, V_h1_proj, V - V_h1_proj), separate_colorbars=True)


As you might have guessed, we have additionally opted here to only use the span of the first 10 basis vectors of trivial_basis. Like NumPy arrays, VectorArrays can be sliced and indexed. The result is always a view onto the original data. If the view object is modified, the original array is modified as well.

Next we will assess the approximation error a bit more thoroughly, by evaluating it on a validation set of 100 parameter values for varying basis sizes.

First, we compute the validation snapshots:

validation_set = parameter_space.sample_randomly(100)
V = fom.solution_space.empty()
for mu in validation_set:
V.append(fom.solve(mu))


To optimize the computation of the projection matrix and the right-hand side for varying basis sizes, we first compute these for the full basis and then extract appropriate sub-matrices:

def compute_proj_errors(basis, V, product):
G = basis.gramian(product=product)
R = basis.inner(V, product=product)
errors = []
for N in range(len(basis) + 1):
if N > 0:
v = np.linalg.solve(G[:N, :N], R[:N, :])
else:
v = np.zeros((0, len(V)))
V_proj = basis[:N].lincomb(v.T)
errors.append(np.max((V - V_proj).norm(product=product)))
return errors

trivial_errors = compute_proj_errors(trivial_basis, V, fom.h1_0_semi_product)


Here we have used the fact that we can form multiple linear combinations at once by passing multiple rows of linear coefficients to lincomb. The norm method returns a NumPy array of the norms of all vectors in the array with respect to the given inner product Operator. When no norm is specified, the Euclidean norms of the vectors are computed.

Let’s plot the projection errors:

from matplotlib import pyplot as plt
plt.figure()
plt.semilogy(trivial_errors)
plt.ylim(1e-1, 1e1)
plt.show() Good! We see an exponential decay of the error with growing basis size. However, we can do better. If we want to use a smaller basis than we have snapshots available, just picking the first of these obviously won’t be optimal.

## Strong greedy algorithm¶

The strong greedy algorithm iteratively builds reduced spaces $$V_N$$ with a small worst-case best approximation error on a training set of solution snapshots by adding, in each iteration, the currently worst-approximated snapshot vector to the basis of $$V_N$$.

We can easily implement it as follows:

def strong_greedy(U, product, N):
basis = U.space.empty()

for n in range(N):
# compute projection errors
G = basis.gramian(product)
R = basis.inner(U, product=product)
lambdas = np.linalg.solve(G, R)
U_proj = basis.lincomb(lambdas.T)
errors = (U - U_proj).norm(product)

# extend basis
basis.append(U[np.argmax(errors)])

return basis


Obviously, this algorithm is not optimized as we keep computing inner products we already know, but it will suffice for our purposes. Let’s compute a reduced basis using the strong greedy algorithm:

greedy_basis = strong_greedy(U, fom.h1_0_product, 25)


We compute the approximation errors for the validation set as before:

greedy_errors = compute_proj_errors(greedy_basis, V, fom.h1_0_semi_product)

plt.figure()
plt.semilogy(trivial_errors, label='trivial')
plt.semilogy(greedy_errors, label='greedy')
plt.ylim(1e-1, 1e1)
plt.legend()
plt.show() Indeed, the strong greedy algorithm constructs better bases than the trivial basis construction algorithm. For compact training sets contained in a Hilbert space, it can actually be shown that the greedy algorithm constructs quasi-optimal spaces in the sense that polynomial or exponential decay of the N-widths $$d_N$$ yields similar rates for the worst-case best-approximation errors of the constructed $$V_N$$.

## Orthonormalization required¶

There is one technical problem with both algorithms however: the condition numbers of the Gramians used to compute the projection onto $$V_N$$ explode:

G_trivial = trivial_basis.gramian(fom.h1_0_semi_product)
G_greedy = greedy_basis.gramian(fom.h1_0_semi_product)
trivial_conds, greedy_conds = [], []
for N in range(1, len(U)):
trivial_conds.append(np.linalg.cond(G_trivial[:N, :N]))
greedy_conds.append(np.linalg.cond(G_greedy[:N, :N]))
plt.figure()
plt.semilogy(range(1, len(U)), trivial_conds, label='trivial')
plt.semilogy(range(1, len(U)), greedy_conds, label='greedy')
plt.legend()
plt.show() This is quite obvious as the snapshot matrix U becomes more and more linear dependent the larger it grows.

If we would use the bases we just constructed to build a reduced-order model from them, we will quickly get bitten by the limited accuracy of floating-point numbers.

There is a simple remedy however: we orthonormalize our bases. The standard algorithm in pyMOR to do so, is a modified gram_schmidt procedure with re-orthogonalization to improve numerical accuracy:

gram_schmidt(greedy_basis, product=fom.h1_0_semi_product, copy=False)
gram_schmidt(trivial_basis, product=fom.h1_0_semi_product, copy=False)


The copy=False argument tells the algorithm to orthonormalize the given VectorArray in-place instead of returning a new array with the orthonormalized vectors.

Since the vectors in greedy_basis and trivial_basis are now orthonormal, their Gramians are identity matrices (up to numerics). Thus, their condition numbers should be near 1:

G_trivial = trivial_basis.gramian(fom.h1_0_semi_product)
G_greedy = greedy_basis.gramian(fom.h1_0_semi_product)

print(f'trivial: {np.linalg.cond(G_trivial)}, '
f'greedy: {np.linalg.cond(G_greedy)}')

trivial: 1.0000000000000038, greedy: 1.000000000000002


Orthonormalizing the bases does not change their linear span, so best-approximation errors stay the same. Also, we can compute these errors now more easily by exploiting orthogonality:

def compute_proj_errors_orth_basis(basis, V, product):
errors = []
for N in range(len(basis) + 1):
v = V.inner(basis[:N], product=product)
V_proj = basis[:N].lincomb(v)
errors.append(np.max((V - V_proj).norm(product)))
return errors

trivial_errors = compute_proj_errors_orth_basis(trivial_basis, V, fom.h1_0_semi_product)
greedy_errors  = compute_proj_errors_orth_basis(greedy_basis, V, fom.h1_0_semi_product)

plt.figure()
plt.semilogy(trivial_errors, label='trivial')
plt.semilogy(greedy_errors, label='greedy')
plt.ylim(1e-1, 1e1)
plt.legend()
plt.show() ## Proper Orthogonal Decomposition¶

Another popular method to create a reduced basis out of snapshot data is the so-called Proper Orthogonal Decomposition (POD) which can be seen as a non-centered version of Principal Component Analysis (PCA). First we build a snapshot matrix

$\begin{split}A := \begin{bmatrix} \vdots & \vdots & \cdots & \vdots \\ u(\mu_1) & u(\mu_2) & \cdots & u(\mu_K)\\ \vdots & \vdots & \cdots & \vdots \end{bmatrix},\end{split}$

where $$K$$ denotes the total number of solution snapshots. Then we compute the SVD of $$A$$

$A = U \Sigma V^T,$

where $$\Sigma$$ is an $$r \times r$$-diagonal matrix, $$U$$ is an $$n \times r$$-matrix and $$V$$ is an $$K \times r$$-matrix. Here $$n$$ denotes the dimension of the solution_space and $$r$$ is the rank of $$A$$. The diagonal entries $$\sigma_i$$ of $$\Sigma$$ are the singular values of $$A$$, which are assumed to be monotonically decreasing. The pairwise orthogonal and normalized columns of $$U$$ and $$V$$ are the left- resp. right-singular vectors of $$A$$. The $$i$$-th POD mode is than simply the $$i$$-th left-singular vector of $$A$$, i.e. the $$i$$-th column of $$U$$. The larger the corresponding singular value is, the more important is this vector for the approximation of the snapshot data. In fact, if we let $$V_N$$ be the span of the first $$N$$ left-singular vectors of $$A$$, then the following error identity holds:

$\begin{split}\sum_{k = 1}^K \inf_{v \in V_N} \|u(\mu_k) - v\|^2 =\, \min_{\substack{W_N \subseteq V\\ \operatorname{dim}(W_N) \leq N}} \sum_{k = 1}^K \inf_{v \in W_N} \|u(\mu_k) - v\|^2 = \sum_{i = N+1}^{r} \sigma^2\end{split}$

Thus, the linear spaces produced by the POD are actually optimal, albeit in a different error measure: instead of looking at the worst-case best-approximation error over all parameter values, we minimize the $$\ell^2$$-sum of all best-approximation errors. So in the mean squared average, the POD spaces are optimal, but there might be parameter values for which the best-approximation error is quite large.

So far we completely neglected that the snapshot vectors may lie in a Hilbert space with some given inner product. To account for that, instead of the snapshot matrix $$A$$, we consider the linear mapping that sends the $$i$$-th canonical basis vector $$e_k$$ of $$\mathbb{R}^K$$ to the vector $$u(\mu_k)$$ in the solution_space:

$\Phi: \mathbb{R}^K \to V, \ e_k \mapsto u(\mu_k).$

Also for this finite-rank (hence compact) operator there exists a SVD of the form

$\Phi(v) = \sum_{i=1}^r u_i \cdot \sigma_i \cdot (v_i, v) \qquad \forall v \in \mathbb{R}^K,$

with orthonormal vectors $$u_i$$ and $$v_i$$ that generalizes the SVD of a matrix.

The POD in this more general form is implemented in pyMOR by the pod method, which can be called as follows:

pod_basis, pod_singular_values = pod(U, product=fom.h1_0_semi_product, modes=25)


We said that the POD modes (left-singular vectors) are orthonormal with respect to the inner product on the target Hilbert-space. Let’s check that:

np.linalg.cond(pod_basis.gramian(fom.h1_0_semi_product))

1.000000000010063


Now, let us compare how the POD performs against the greedy algorithm in the worst-case best-approximation error:

pod_errors = compute_proj_errors_orth_basis(pod_basis, V, fom.h1_0_semi_product)

plt.figure()
plt.semilogy(trivial_errors, label='trivial')
plt.semilogy(greedy_errors, label='greedy')
plt.semilogy(pod_errors, label='POD')
plt.ylim(1e-1, 1e1)
plt.legend()
plt.show() As it turns out, the POD spaces perform even slightly better than the greedy spaces. Why is that the case? Note that for finite training or validation sets, both considered error measures are equivalent. In particular:

$\sup_{k = 1,\ldots,K} \inf_{v \in V_N} \|u(\mu_k) - v\| \leq \left[\sum_{k = 1}^K \inf_{v \in V_N} \|u(\mu_k) - v\|^2\right]^{1/2} \leq \sqrt{K} \cdot \sup_{k = 1,\ldots,K} \inf_{v \in V_N} \|u(\mu_k) - v\|.$

Since POD spaces are optimal in the $$\ell^2$$-error, they miss the error of the optimal space in the Kolmogorov sense by at most a factor of $$\sqrt{K}$$, which in our case is $$5$$. On the other hand, the greedy algorithm also only produces quasi-optimal spaces. – For very large training sets with more complex parameter dependence, differences between both spaces may be more significant.

Finally, it is often insightful to look at the POD modes themselves:

fom.visualize(pod_basis)