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We introduce on the domain $\Omega = (0,1)$ a mesh $0=x_0<x_1<x_2<\dots<x_{n+1}=1$ and let $V_h$ be the space of piecewise linear hat functions $\varphi_i$ such that

$$\varphi_i'= \left\{ \begin{array}{ll} \frac{1}{x_i-x_{i-1}}=\frac{1}{h_i}, & \quad x_{i-1}<x<x_i \\ \frac{-1}{x_{i+1}-x_{i}}=-\frac{1}{h_{i+1}}, & \quad x_{i}<x<x_{i+1} \\ 0, & \quad\text{ otherwise} \end{array} \right. $$

We can then easily compute the corresponding stiffness matrix $K$ and mass matrix $M$ by evaluating the integrals below,

$$K_{ij}:=(\varphi_i', \varphi_j') = \int_0^1 \varphi'_i\varphi'_jdx$$ $$M_{ij}:=(\varphi_i, \varphi_j) = \int_0^1 \varphi_i\varphi_jdx$$

So that

$$K_{ij} = (\varphi_i', \varphi_j') = \left\{ \begin{array}{ll} -\frac{1}{h_i}, & \quad j=i-1 \\ \frac{1}{h_i} + \frac{1}{h_{i+1}}, & \quad j=i \\ \frac{-1}{h_{i+1}}, & \quad j=i+1 \\ 0, & \quad\text{ otherwise} \end{array} \right.$$

$$M_{ij} = (\varphi_i, \varphi_j) = \left\{ \begin{array}{ll} \frac{1}{6}h_i, & \quad j=i-1 \\ \frac13({h_i} +{h_{i+1}}), & \quad j=i \\ \frac16 h_{i+1}, & \quad j=i+1 \\ 0, & \quad\text{ otherwise} \end{array} \right.$$

What I don't understand in this example is how actually the values $K_{ij}$ and $M_{ij}$ were obtained. Let me explain what I mean:

Let $x\in (x_{i-1}, x_i)$, then

$$K_{ij}=(\varphi_i', \varphi_j')=\int_0^1 \varphi_i'\varphi_j' dx =\int_0^1 \frac{1}{h_i}\frac{1}{h_j}dx=\frac{1}{h_i h_j}=\frac{1}{h_i^2},$$ which does not coincide with what is in the book.

What is it that I'm misunderstanding?

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The piecewise linear hat function $\;\phi_i\;$ itself is: $$ \phi_i(x)= \left\{ \begin{matrix} (x-x_{i-1})/(x_i-x_{i-1}) & \quad \text{for} \quad x_{i-1} < x < x_i \\ (x_{i+1}-x)/(x_{i+1}-x_{i}) & \quad \text{for} \quad x_{i}< x < x_{i+1} \\ 0 & \quad \text{ otherwise} \end{matrix} \right. $$ But I think that the mass matrix is given instead by the integral below: $$ M_{i,j}:=(\phi_i, \phi_j) = \int_{x_{i-1}}^{x_{i+1}} \phi_i(x)\phi_j(x)\;dx $$ Three non-zero cases (make a sketch): $$ M_{i,i-1} = \int_{x_{i-1}}^{x_{i+1}} \phi_i(x)\phi_{i-1}(x)\;dx = \\ \frac{1}{(x_i-x_{i-1})^2} \int_{x_{i-1}}^{x_i} (x-x_{i-1})(x_{i}-x)\;dx = \frac{x_i-x_{i-1}}{6} $$ $$ M_{i,i+1} = \int_{x_{i-1}}^{x_{i+1}} \phi_i(x)\phi_{i+1}(x)\;dx = \\ \frac{1}{(x_{i+1}-x_{i})^2} \int_{x_{i}}^{x_{i+1}} (x-x_{i+1})(x_{i}-x)\;dx = \frac{x_{i+1}-x_{i}}{6} $$ $$ M_{i,i} = \int_{x_{i-1}}^{x_{i+1}} \phi_i(x)\phi_{i}(x)\;dx = \\ \frac{1}{(x_{i}-x_{i-1})^2} \int_{x_{i-1}}^{x_{i}} (x-x_{i-1})^2\;dx +\frac{1}{(x_{i+1}-x_{i})^2} \int_{x_{i}}^{x_{i+1}} (x_{i+1}-x)^2\;dx = \frac{x_{i+1}-x_{i-1}}{3} $$ Suppose that also the stiffness matrix is given instead by the integral below: $$ K_{i,j}:=(\phi_i', \phi_j') = \int_{x_{i-1}}^{x_{i+1}} \phi'_i(x)\phi'_j(x)\;dx $$ Then can you do this part of the exercise yourself?

I wouldn't be much surprised if the confusion is due to a typo in your book: a mix up of local and global coordinates could be the case. The following two references at MSE seem to be related to your question and might be helpful:

  1. Understanding Galerkin method of weighted residuals
  2. Are there any two-dimensional quadrature that only uses the values at the vertices of triangles?
.

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Imagine that $x_i$ is an interior node: then $\varphi_i$ is nonzero only in the interval $(x_{i-1},x_{i+1})$, and the same happens with $\varphi_i'$. The integral is computed over $(0,1)$ but the functions are nonzero in smaller intervals.

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  • $\begingroup$ Thanks, but then $\int_0^1 \frac{1}{h_i} \frac{1}{h_j}dx = \int_{x_{i-1}}^{x_i} \frac{1}{h_i} \frac{1}{h_j}dx+ \int_{x_{i}}^{x_{i+1}} \frac{1}{h_i} \frac{1}{h_j}dx=0$ because the integrands are products of functions which are only defined on their respective intervals. Isn't this true? $\endgroup$ – sequence Apr 8 at 20:44

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