diff --git a/doc/gendoc.py b/doc/gendoc.py index f552c4e0..6e6f07b7 100755 --- a/doc/gendoc.py +++ b/doc/gendoc.py @@ -45,6 +45,8 @@ f = open('plugins_generated.tex', 'w') f.write('\section{Plugin reference}\n') f.write('\input{section_bsdf}\n') os.path.walk('../src/bsdfs', traverse, f) +f.write('\input{section_integrators}\n') +os.path.walk('../src/integrators', traverse, f) f.close() os.system('bibtex main.aux') os.system('pdflatex main.tex') diff --git a/doc/images/glass_explanation.ai b/doc/images/glass_explanation.ai new file mode 100644 index 00000000..ddc55640 --- /dev/null +++ b/doc/images/glass_explanation.ai @@ -0,0 +1,1077 @@ +%PDF-1.5 % +1 0 obj <>/OCGs[7 0 R 34 0 R]>>/Pages 3 0 R/Type/Catalog>> endobj 2 0 obj <>stream + + + + + application/pdf + + + Web + + + + + Adobe Illustrator CS5 + 2011-07-01T22:52:28+02:00 + 2011-07-01T23:53:23+02:00 + 2011-07-01T23:53:23+02:00 + + + + 256 + 112 + JPEG + /9j/4AAQSkZJRgABAgEASABIAAD/7QAsUGhvdG9zaG9wIDMuMAA4QklNA+0AAAAAABAASAAAAAEA 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To achieve realistic results, Mitsuba -comes with a library of both general-purpose models (smooth or rough glass, -metal, plastic, etc.) and specializations to particular materials -(woven cloth, masks, etc.). +\label{sec:bsdfs} +Surface scattering models describe the manner in which light interacts +with surfaces in the scene. They conveniently summarize the mesoscopic +scattering processes that take place within the material and +cause it to look the way it does. +This represents one central component of the material system in Mitsuba---another +part of the renderer concerns itself with what happens +\emph{in between} surface interactions. For more information on this aspect, +please refer to Sections~\ref{sec:media} and \ref{sec:subsurface}. +This section presents an overview of all surface scattering models that are +supported, along with their parameters. -Throughout the documentation and within the scene description language, -the word \emph{BSDF} is used synonymously with the term ``surface -scattering model''. This is an abbreviation for \emph{Bidirectional +\subsubsection*{Correctness considerations} +\begin{figure}[b!] +\centering +\vspace{-5mm} +\includegraphics[width=15cm]{images/glass_explanation.pdf} +\vspace{-5mm} +\caption{ + \label{fig:glass-explanation} + Some of the scattering models in Mitsuba need to know + the indices of refraction on the exterior and interior-facing + side of a surface. + It is therefore important to decompose the mesh into meaningful + separate surfaces corresponding to each index of refraction change. + The example here shows such a decomposition for a water-filled Glass. +} +\end{figure} + + +A vital consideration when modeling a scene in a physically-based rendering +system is that the used materials do not violate physical properties, and +that their arrangement is meaningful. For instance, imagine having designed +an architectural interior scene that looks good except for a white desk that +seems a bit too dark. A closer inspection reveals that it uses a Lambertian +material with a diffuse reflectance of $0.9$. + +In many rendering systems, it would be feasible to increase the +reflectance value above $1.0$ in such a situation. But in Mitsuba, even a +small surface that reflects a little more light than it receives will +likely break the available rendering algorithms, or cause them to produce otherwise +unpredictable results. In fact, we should rather change the lighting setup and +then \emph{reduce} the material's reflectance, since it is quite unlikely that +we could find a real-world desk with a reflectance as high as $0.9$. + +As an example of the necessity for a meaningful material arrangement, consider +the glass model illustrated in \figref{glass-explanation}. Here, careful thinking +is needed to decompose the object into boundaries that mark index of +refraction-changes. If this is done incorrectly and a beam of light can +potentially pass through a sequence of incompatible index of refraction changes (e.g. $1.00\to 1.33$ +followed by $1.50\to1.33$), the output is undefined and will quite likely +even contain inaccuracies in parts of the scene that are some distance +away from the glass. + +\subsubsection*{BSDFs} +To achieve realistic results, Mitsuba comes with a library of both +general-purpose surface scattering models (smooth or rough glass, metal, +plastic, etc.) and specializations to particular materials (woven cloth, +masks, etc.). Some model plugins fit neither category and could be described +as \emph{modifiers} that are applied on top of one or more scattering models. + +Throughout the documentation and within the scene description +language, the word \emph{BSDF} is used synonymously with the term ``surface +scattering model''. This is an abbreviation for \emph{Bidirectional Scattering Distribution Function}, a more precise technical -description of the model's properties. In Mitsuba, BSDFs are +term. + +In Mitsuba, BSDFs are assigned to \emph{shapes}, which describe the visible surfaces in the scene. In the scene description language, this assignment can either be performed by nesting BSDFs within shapes, or they can -be named and then later referenced by their name. - +be named and then later referenced by their name. The following fragment shows an example of both kinds of usages: \begin{xml} @@ -26,13 +81,11 @@ The following fragment shows an example of both kinds of usages: - - - + @@ -42,3 +95,4 @@ The following fragment shows an example of both kinds of usages: It is generally more economical to use named BSDFs when they are used in several places, since this reduces Mitsuba's internal memory usage. + diff --git a/doc/section_integrators.tex b/doc/section_integrators.tex new file mode 100644 index 00000000..31eaf587 --- /dev/null +++ b/doc/section_integrators.tex @@ -0,0 +1,88 @@ +\newpage +\subsection{Integrators} +\label{sec:integrators} +In Mitsuba, the different rendering techniques are collectively referred to as +\emph{integrators}, since they perform integration over a high-dimensional +space. Each integrator represents a specific approach for solving +the light transport equation---usually favored in certain scenarios, but +at the same time affected by its own set of intrinsic limitations. +Therefore, it is important to carefully select an integrator based on +user-specified accuracy requirements and properties of the scene to be +rendered. + +In Mitsuba's XML description language, a single integrator +is usually instantiated by declaring it at the top level within the +scene, e.g. +\begin{xml} + + + + + + + + + + + +\end{xml} + +This section gives a brief overview of the available choices +along with their parameters. + +\subsubsection*{Path length} +\begin{figure}[htb!] +\centering +\hfill +\smallrendering{Max. length = 1}{pathlength-1} +\smallrendering{Max. length = 2}{pathlength-2} +\smallrendering{Max. length = 3}{pathlength-3} +\smallrendering{Max. length = $\infty$}{pathlength-all} +\caption{ + \label{fig:pathlengths} + These Cornell box renderings demonstrate the visual + effect of a maximum path length. As the paths + are allowed to grow longer, the color saturation + increases due to multiple scattering interactions + with the colored surfaces. At the same time, the + computation time increases. +} +\end{figure} + +Almost all integrators use the concept of \emph{path length}. +Here, a path refers to a chain of scattering events that +starts at the light source and ends at the eye or camera. +It is often useful to limit the path length (\figref{pathlengths}) +when rendering scenes for preview purposes, since this reduces the amount +of computation that is necessary per pixel. Furthermore, such renderings +usually converge faster and therefore need fewer samples per pixel. +When reference-quality is desired, one should always leave the path +length unlimited. + +\begin{figure}[h!] +\centering +\vspace{-5mm} +\includegraphics[width=10cm]{images/path_explanation.pdf} +\vspace{-5mm} +\caption{ + \label{fig:path-explanation} + A ray of emitted light is scattered by an object and subsequently + reaches the eye/camera. + In Mitsuba, this is a \emph{length-2} path, since it has two edges. +} +\end{figure} +Mitsuba counts lengths starting at $1$, which correspond to +visible light sources (i.e. a path that starts at the light +source and ends at the eye or camera without any scattering +interaction in between). +A length-$2$ path (also known as ``direct illumination'') includes +a single scattering event (\figref{path-explanation}). + +\subsubsection*{Progressive versus non-progressive} +Some of the rendering techniques in Mitsuba are \emph{progressive}. +What this means is that they display a rough preview, which +improves over time. Leaving them running indefinitely will +continually reduce noise (e.g. in Metropolis Light Transport) +or both noise and bias (e.g. in Progressive Photon Mapping). + diff --git a/schema/scene.xsd b/schema/scene.xsd index 10ac544a..162a9125 100644 --- a/schema/scene.xsd +++ b/schema/scene.xsd @@ -26,6 +26,7 @@ + diff --git a/src/bsdfs/dielectric.cpp b/src/bsdfs/dielectric.cpp index a6984895..b8ae02d7 100644 --- a/src/bsdfs/dielectric.cpp +++ b/src/bsdfs/dielectric.cpp @@ -28,14 +28,21 @@ MTS_NAMESPACE_BEGIN * \parameter{extIOR}{\Float}{Exterior index of refraction \default{1.0}} * \parameter{specular\showbreak Reflectance}{\Spectrum\Or\Texture}{Optional * factor used to modulate the reflectance component\default{1.0}} - * \parameter{specular\showbreak Transmittance}{\Spectrum\Or\Texture}{Optional + * \lastparameter{specular\showbreak Transmittance}{\Spectrum\Or\Texture}{Optional * factor used to modulate the transmittance component\default{1.0}} * } * - * Models an interface between two materials with non-matched indices of refraction. - * The microscopic surface structure is assumed to be perfectly flat, resulting - * in a BSDF equal to a Dirac delta function. - * The default settings are set to a borosilicate glass BK7/air interface. + * This plugin models an interface between two materials having mismatched + * indices of refraction (e.g. a boundary between water and air). + * The microscopic surface structure of the surface is assumed to be perfectly + * smooth, resulting in a degenerate BSDF described by a Dirac delta function. + * For non-smooth interfaces, please take a look at the \pluginref{roughglass} + * model. When using this plugin, it is crucial that the scene contains + * meaningful and mutally compatible index of refraction change -- see + * \figref{glass-explanation} for an example. + * + * The default settings of this plugin are set to a borosilicate glass BK7/air + * interface. */ class Dielectric : public BSDF { public: diff --git a/src/bsdfs/roughglass.cpp b/src/bsdfs/roughglass.cpp index b2cc43d0..377d9e36 100644 --- a/src/bsdfs/roughglass.cpp +++ b/src/bsdfs/roughglass.cpp @@ -73,6 +73,10 @@ MTS_NAMESPACE_BEGIN * distributions and a texturable roughness. The default settings are set * to a borosilicate glass BK7/air interface with a light amount of rougness * modeled using a Beckmann distribution. + * + * When using this plugin, it is crucial that the scene contains + * meaningful and mutally compatible index of refraction change -- see + * \figref{glass-explanation} for an example. */ class RoughGlass : public BSDF { public: diff --git a/src/integrators/path/path.cpp b/src/integrators/path/path.cpp index 783c3656..684fcc69 100644 --- a/src/integrators/path/path.cpp +++ b/src/integrators/path/path.cpp @@ -23,19 +23,26 @@ MTS_NAMESPACE_BEGIN static StatsCounter avgPathLength("Path tracer", "Average path length", EAverage); - /** - * Extended path tracer -- uses multiple importance sampling to combine - * two sampling strategies, namely BSDF and luminaire sampling. - * This class does not attempt to solve the full radiative transfer - * equation (see volpath if this is needed). - */ +/*! \plugin{path}{Path tracer with multiple importance sampling} + * \parameters{ + * \parameter{maxDepth}{\Integer}{Maximum path depth \default{-1}} + * \parameter{strictNormals}{\Boolean}{Strict normals?} + * } + * Extended path tracer -- uses multiple importance sampling to combine + * two sampling strategies, namely BSDF and luminaire sampling. + * This class does not attempt to solve the full radiative transfer + * equation (see volpath if this is needed). + */ class MIPathTracer : public MonteCarloIntegrator { public: - MIPathTracer(const Properties &props) : MonteCarloIntegrator(props) { } + MIPathTracer(const Properties &props) + : MonteCarloIntegrator(props) { + //m_shadingSamples = props.getInteger("shadingSamples"); + } /// Unserialize from a binary data stream MIPathTracer(Stream *stream, InstanceManager *manager) - : MonteCarloIntegrator(stream, manager) { } + : MonteCarloIntegrator(stream, manager) { } Spectrum Li(const RayDifferential &r, RadianceQueryRecord &rRec) const { /* Some aliases and local variables */