This coursework is due on:
Fri Oct 27th at 22:00
Submisssion is via github.
I will be doing incremental testing starting from Fri 20th, but only based on what you currently have in your github private repo. When exactly that testing happens will be sporadic and unpredictable (no more than once a day), both by intention (to avoid dependency on a perceived "deadline") and necessity (I have to kick it off manually).
The process I'll follow is:
-
Clone from your "master" branch
-
Run tests on my local setup and record results
-
Push the results back into a folder called
dt10_logs
in your private repository.
It is up to you to keep your repository in a compilable state. You can do this by either:
1 - Collecting commits locally until you are happy with a "release" you want to push.
2 - Using a "dev" branch to handle speculative development, then push to the "master" branch when you reach milestones.
This coursework explores parallelism using threaded-building blocks in a bit more detail. You should see linear speedup here in a slightly more complex example than in CW1, i.e. the performance rises in proportion to the number of CPU cores.
This distribution contains a basic object framework for creating and using fourier transforms, as well as two implementations:
- A direct fourier transform taking O(n^2) steps.
- A recursive fast-fourier transform taking O(n log n) steps.
Also included within the package is a very simple test suite to check that the transforms work, and a registry which allows new transforms to be added to the package.
Your job in this coursework is to explore a number of basic (but effective) ways of using TBB to accelerate existing code, and to compare and contrast the performance benefits of them.
Dislaimer: Never write your own fourier transform for production use. Everything you do here will be slower and less accurate than existing FFT libraries.
You may notice that this used to be CW3 a few years ago, but is now CW2. This is to reflect the change in order and emphasis compared to previous years. The older matlab experiment (which was awesome, but no-one liked matlab) has disappeared in favour of the very simple TBB intro in CW1, with this experiment to elaborate the TBB approach and explore it in a bit more detail. There is also more emphasis on exploring performance, as I think that previously people focussed on just getting the code working. There are quite a few graphs to get (five), but if you follow the advice about how to automate things, it is fairly quick to get them.
You can select your environment in a similar way to CW1, but the assessed compilation and evaluation will be done under Ubuntu in AWS. My plan is to use a c4.8xlarge instance, but you don't need to optimise your code specifically for that machine. This shouldn't matter to you now (as you're not relying on anything apart from TBB), but is more encouragement to try out AWS before you have to later on.
Submission will be via github, so this time you'll need
to actually work with your private repository. I have created
you a private repository again, but this time it will be empty.
It is up to you clone
a local copy of the master repository,
then push
it back up to your private repository. There
are more details on this in the brief git intro.
Also.
Note: It is not a disaster if submission via github doesn't work, as I will also be getting people to do a blackboard submission as backup so I get the code. However, I did this for the last three years, and it worked fine.
The package you have been given is a slightly overblown
framework for implementing fourier transforms. The file
include\fourier_transform.hpp
defines a generic
fourier transform interface, allowing forwards and
backwards transforms.
In the src directory, there are two fourier transform implementations, and two programs:
-
test_fourier_transform
, which will run a number of simple tests on a given transform to check it works. The level of acceptable error in the results is defined as 1e-9 (which is quite high). -
time_fourier_transform
, which will time a given transform for increasing transform sizes with a given level of allowed parallelism.
If you build the two programs use:
make all
then you should be able to test and time the two existing transforms. For example, you can do:
bin/test_fourier_transform
which will list the two existing transforms, and:
bin/time_fourier_transform hpce.fast_fourier_transform
to see the effect of increasing transform size on
execution time (look in time_fourier_transform.cpp
to
see what the columns mean).
Even though there is no parallelism in the default framework, it still relies on TBB to control parallelism, so it will not build, link, or execute, without TBB being available.
Note: the direct fourier transform is very likely to fail a small number of tests, while the fast fourier transform should pass all of them. This demonstrates that even though two algorithms calculate the same result, the order of calculation can change the numerical accuracy significantly. In case you are not aware, floating point is not exact, and if you add together long sequences the error adds up quickly.
You may wish to consider the algorithmic tradeoffs
between the sequential direct and fast fourier
transforms - what is an achievable n
for the
direct versus the fast transform. Remember that
parallelism and optimisation are never a substitute
for an algorithm with a better intrinsic complexity.
The file src/direct_fourier_transform.cpp
contains a classic
discrete fourier transform, which takes O(n^2) operations to
do an n-point fourier transform. Classic 1st year maths :)
First we're going to parallelise the inner loop, in order to directly observe the overheads of parallelisation.
The framework is designed to support multiple fourier
transforms which you can select between, so we'll
need a way of distinguishing your transform from
anyone else's (in principle I should be able to create
one giant executable containing everyone in the
class's transforms). The basic framework uses the namespace
hpce
, but your classes will live in the namespace
hpce::your_login
, and the source files in src/your_login
.
For example, my namespace is hpce::dt10
, and my
source files go in src/dt10
.
There are five steps in this process:
- Creating the new fourier transform class
- Registering the class with the fourier framework
- Adding the parallel constructs to the new class
- Testing the parallel functionality (up to you)
- Finding the new execution time (up to you, see notes at the end).
Copy src/direct_fourier_transform.cpp
into a new
file called src/your_login/direct_fourier_transform_parfor_inner.cpp
.
Modify the new file so that the contained class is called
hpce::your_login::direct_fourier_transform_parfor_inner
, and reports
hpce.your_login.direct_fourier_transform_parfor_inner
from name()
. Apart
from renaming, you don't need to change any functionality yet.
To declare something in a nested namespace, simply
insert another namespace declaration inside the existing
one. For example, if you currently have hpce::my_class
:
namespace hpce{
class my_class{
...
};
};
you could get it into a new namespace called bobble, by changing it to:
namespace hpce{
namespace bobble{
class my_class{
...
};
};
};
which would result in a class with the name hpce::bobble::my_class
.
Add your new file to the set of objects compiled into
the executable by adding it to FOURIER_IMPLEMENTATION_OBJS
in the makefile
,
and check that it still compiles.
As part of the modifications, you probably noticed
a function at the bottom of the file called std::shared_ptr<fourier_transform> Create_direct_fourier_transform()
,
and (hopefully!) modified to std::shared_ptr<fourier_transform> Create_direct_fourier_transform_parfor_inner()
.
This is the factory function, used by the rest of the
framework to create transforms by name, without knowing
how they are implemented.
If you look in src/fourier_transform_register_factories.cpp
, you'll
see a function called fourier_transform::RegisterDefaultFactories
,
which is where you can register new transforms. To minimise
compile-time dependencies, the core framework knows nothing
about the transforms - all it knows is how to create them.
Towards the top is a space to declare your external factory
function, which can be uncommented. Then at the bottom
of RegisterDefaultFactories
, uncomment the call which
registers the factory.
At this point, you should find that your new implementation
is listed if you build test_fourier_transform
and run it with no
arguments:
bin/test_fourier_transform
For example, I get:
$ bin/test_fourier_transform
hpce.direct_fourier_transform
hpce.dt10.direct_fourier_transform_parfor_inner
hpce.fast_fourier_transform
You can now test it or time it:
bin/test_fourier_transform hpce.[your_login].direct_fourier_transform_parfor_inner
or:
bin/time_fourier_transform hpce.[your_login].direct_fourier_transform_parfor_inner
Hopefully your implementation still works, in so far as the execution will be identical, and the time should be the same (beyond run-to-run variations due to the system).
If your transform doesn't turn up at run-time, or the code won't compile,
make very sure that you have renamed everything within
src/your_login/direct_fourier_transform_parfor_inner.cpp
to the
new name. Also make sure that the factory function is declared
as std::shared_ptr<fourier_transform> hpce::your_login::Create_direct_fourier_transform_parfor_inner()
,
both in src/your_login/direct_fourier_transform_parfor_inner.cpp
, and in
src/fourier_transform_register_factories.cpp
(particularly if you get a linker error).
You need to rewrite the inner loop in both forwards_impl
and backwards_impl
,
using the transformation of for loop to tbb::parallel_for
shown previously. I would
suggest doing one, running the tests, and then doing the other. You'll
need to make sure that you include the appropriate header for parallel_loop from
TBB at the top of the file, so that the function can be found.
We are now going to explore tuning the grain size, which is essentially adjusting the ratio of computation to parallel overhead. This should provide much more explicit versions of the tradeoffs that you may have seen in the previous coursework.
By default, tbb::parallel_for
uses something called
the auto_partitioner
, which is used to partition
your iteration space into parallel chunks. The auto-partitioner
attempts to balance the number of parallel tasks created
against the amount of computation at each iteration
point. Internally it tries to split the iteration space
up recursively into parallel chunks, and then switches
to serial execution within each chunk once it has enough
parallel tasks for the number of processors.
We can explore this and control it by using manual grain size control, which explicitly says how big each parallel task should be. There is an alternate form of parallel_for, which describes a chunked iteration space:
tbb::parallel_for(tbb::blocked_range<unsigned>(i,j,K), [&](const tbb::blocked_range<unsigned> &chunk){
for(unsigned i=chunk.begin(); i!=chunk.end(); i++ ){
y[i]=myLoop(i);
}
}, tbb::simple_partitioner());
This is still equivalent to the original loop, but now we have more control. If we unpack it a bit, we could say:
// Our iteration space is over the unsigneds
typedef tbb::blocked_range<unsigned> my_range_t;
// I want to iterate over the half-open space [i,j),
// and the minimum parallel chunk size should be K.
my_range_t range(i,j,K);
// This will apply my function over the half-open
// range [chunk.begin(),chunk.end) sequentially.
auto f=[&](const my_range_t &chunk){
for(unsigned i=chunk.begin(); i!=chunk.end(); i++ ){
y[i]=myLoop(i);
}
};
We now have the choice of executing it directly:
f(range); // Apply f over range [i,j) sequentially
or in parallel with chunk size of K:
tbb::parallel_for(range, f, tbb::simple_partitioner());
The final tbb::simple_partitioner()
argument is telling
TBB "I know what I am doing; I have decided that K is the
best chunk size."
We could alternatively use tbb::auto_partitioner, which would tell TBB "I know that the chunk size should not be less than K, but if you want to do larger chunks, go for it." In general auto_partitioner will provide better adaptive performance, but for now we want to see where the bad performance occurs.
We want to vary the chunk size, but we also want it to be user tunable for a specific machine. So we are going to allow the user to choose a value K at run-time using an environment variable.
The function getenv
allows a program to read environment variables
at run-time. So if I choose an environment variable called HPCE_X
, I could
create a C++ program read_x
:
#include <cstdlib>
int main()
{
char *v=getenv("HPCE_X");
if(v==NULL){
printf("HPCE_X is not set.\n");
}else{
printf("HPCE_X = %s\n", v);
}
return 0;
}
then on the command line I could do:
> ./read_x
HPCE_X is not set.
> export HPCE_X=wibble
> ./read_x
HPCE_X = wibble
> export HPCE_X=100
> ./read_x
HCPE_X = 100
Environment variables are a way of defining ambient properties,
and are often used for tuning the execution of a program for the
specific machine they are on (I'm not saying it's the best way,
but it happens a lot). I used the HPCE_
prefix as I want to
try to avoid clashes with other programs that might want a
variable called X
.
Modify your implementation of direct_fourier_transform_parfor_inner
to use a chunk size K, where K is either
specified as a decimal integer using the environment
variable HPCE_DIRECT_INNER_K
. If it is not set, you should use
a sensible default. For example, if the user does:
export HPCE_DIRECT_INNER_K=16
you would use a chunk size of 16 for the inner loop.
Hint: in order to save you time: atoi can turn a string into an integer.
You should think about what "sensible default" means: the TBB user guide gives some guidance in the form of a "rule of thumb". Your rule of thumb should probably take into account the approximate amount of work per inner iteration point, so you don't want to choose K=1. However, you would like to eventually have some parallelism, so you also can't choose a really large default K.
Task: create a graph called results/direct_inner_versus_k.pdf
which
explores the performance of K=[1..16] versus time for n=[64,256,1024,4096].
K should be on the x-axis, time on the y-axis, and each n is a different line.
Time should extend up to 30 seconds per test run, which you can achieve with:
export HPCE_DIRECT_INNER_K = <Whatever K you want>
bin/time_fourier_transform hpce.direct_fourier_transform_parfor_inner 0 30
You can generate this file manually by running the program 16 times, picking out the values and putting them in a spreadsheet, or you might want to explore automation further using scripting and pivot charts.
You should be seeing different performance as you scale K (up to a point), and hopefully be developing an intuition that the inner loop is probably not where you want to accelerate in general (unless loop-carried dependencies force you to).
Create a new implementation called direct_fourier_transform_parfor_outer
(with all the associated files and factory setup), and parallelise
over the outer loop.
Be very careful to test your output, and don't blindly assume that things are correct. You may want to look carefully at what the two loops are doing, and how they interact:
-
Can you convert from accumulation into an array to accumulation into a scalar?
-
Think about the 2d iteration space and the dependencies within it.
-
Can you interchange the loops (iterate over a different dimension of the iteration space as the outer loop)?
Task: create a graph called results/direct_outer_time_versus_p.pdf
which
explores the parallelism versus time for varying n.
n should be on the x-axis, time on the y-axis, and each P is a different line
(try to find a machine with at least 4 processors). Again, time should extend up to 30 seconds per test run.
Task: create a graph called results/direct_outer_strong_scaling.pdf
which
explores the scaling with P processors. So the graph should have P on
the x-axis, "scaling" on the y-axis, and have a line for n=[64,256,1024].
Again, try to find a machine with at least 4 cores (it doesn't have
to be the machine in front of you...)
Here we will define "scaling" as follows:
T_S = Time taken for sequential version
T_1 = Time taken for parallel version with one processor
T_P = Time taken for parallel version with P processors
S = T_S / (T_P * P)
Linear scaling would mean than S=1, so we added P processors and it is P times faster. Sub-linear scaling means that S<1, so we are not getting as much out of each additional processor.
Note that I'm defining scaling against T_S, which is the original sequential version with no overhead from TBB. It is entirely possible (and likely) that T_S / T_1 < 1. This is just the principle that nothing comes for free. In order to go parallel, we have to pay something for the libraries.
The file src/fast_fourier_transform.cpp
contains a radix-2
fast fourier transform, which takes O(n log n) operations to
do a transform. There are two main opportunities for parallelism
in this algorithm, both in recurse()
:
-
The recursive splitting, where the function makes two recursive calls to itself.
-
The iterative joining, where the results from the two recursive calls are joined together.
We will first exploit just the recursive splitting using
tbb::task_group
.
Task groups allow us to specify sets of heterogenous
tasks that can run in parallel - by heterogenous, we
mean that each of the tasks can run different code and
perform a different function, unlike parallel_for
where
one function is used for the whole iteration space.
Task groups are declared as an object on the stack:
#include "tbb/task_group.h"
// Within some function, create a group
tbb::task_group group;
you can then add tasks to the group dynamically, using anything which looks like a nullary (zero-input) function as the starting point:
unsigned x=1, y=2;
group.run( [&x](){ x=x*2; } );
group.run( [&y](){ y=y+2; } );
After this code runs, we can't say anything about the values of x and y, as each one has been captured by reference (the [&]) but we don't know if they have been modified yet. It is possible that zero, one, or both of the tasks have completed, so to rejoin the tasks and synchronise we need to do:
group.wait();
After this function executes, all tasks in the group must have finished, so we know that x==2 and y==4.
An illegal use of this construct would be for both tasks to have a reference to x:
// don't do this
unsigned x=7;
group.run( [&x](){ x=x*2; } );
group.run( [&x](){ x=x+2; } );
group.wait();
Because both tasks have a reference to x, any changes in one task are visible in the other task. We don't know what order the two tasks will run in, so the output could be one of:
- x == (7*2)+2
- x == (7+2)*2
- x == 7*2
- x == 7+2
This would be a case of a data-race condition, which is why you should never have two threads sharing the same memory.
Copy src/fast_fourier_transform.cpp
into a new
file called src/your_login/fast_fourier_transform_taskgroup.cpp
.
Modify the new file so that the contained class is called
hpce::your_login::fast_fourier_transform_taskgroup
, and reports
hpce.your_login.fast_fourier_transform_taskgroup
from name(). Apart
from renaming, you don't need to change any functionality yet.
As before, register the implementation with the implementation
in src/fourier_transform_register_factories.cpp
, and check that
the transform still passes the test cases.
In the fast fourier transform there is a natural splitting recursion in the section:
recurse(m,wn*wn,pIn,2*sIn,pOut,sOut);
recurse(m,wn*wn,pIn+sIn,2*sIn,pOut+sOut*m,sOut);
Modify the code to use tbb::task_group to turn the two calls into child tasks. Don't worry about efficiency yet, and keep splitting the tasks down to the point of individual elements - splitting down to individual elements is the wrong thing to do, as it introduces masses of overhead, but we are establishing a base-case here.
As before, test the implementation to make sure it still works.
Our recursive parallel FFT is currently splitting down to individual tasks, which goes against the TBB advice about the minimum work per task:
A rule of thumb is that grainsize iterations of operator() should take at least 100,000 clock cycles to execute. For example, if a single iteration takes 100 clocks, then the grainsize needs to be at least 1000 iterations.
Go back into src/your_login/fast_fourier_transform_taskgroup.cpp
and make the base-case adjustable using the environment variable
HPCE_FFT_RECURSION_K
. This should adjust things at run-time,
so that if I choose:
export HPCE_FFT_RECURSION_K=2
then the work is split down to a two-point serial FFT, while if we do:
export HPCE_FFT_RECURSION_K=16
then the implementation will stop parallel recursion for at a size of 16, and switch to serial recursion (i.e. normal function calls).
You don't want the overhead of calling getenv
all over the
place, so I would suggest calling it once at construction
time and caching it in a member variable for the lifetime
of the FFT instance.
Note: this is an in-place modification, rather than a new class.
Task: : Create a graph called results/fast_fourier_time_vs_recursion_k.pdf
. This
should have n on the x-axis, time on the y-axis, and lines for K=[2,4,8,16,32,64].
The FFT contains a for loop which at first glance appears to be impossible to parallelise, due to the loop carried dependency through w:
std::complex<double> w=std::complex<double>(1.0, 0.0);
for (size_t j=0;j<m;j++){
std::complex<double> t1 = w*pOut[m+j];
std::complex<double> t2 = pOut[j]-t1;
pOut[j] = pOut[j]+t1;
pOut[j+m] = t2;
w = w*wn;
}
However, we can in fact parallelise this loop as long as we exploit some mathematical properties (which should be your forte!) and batch things carefully. On each iteration the loop calculates w=w*wn, so if we look at the value of w at the start of each iteration we have:
j=0
,w=1
j=1
,w=1 * wn
j=2
,w=1 * wn * wn
Generalising, we find that for iteration j, w=wn^j
.
Hopefully it is obvious that raising something to the
power of i takes substantially less than i operations.
Try calculating (1+1e-10)^1e10
in matlab, and notice:
- It is almost equal to e. Nice.
- It clearly does not take anything like 1e10 operations to calculate.
In C++ the std::complex
class supports the std::pow
operator,
which will raise a complex number to a real scalar, which
can be used to jump ahead in the computation. In principle
we could use this property to make the loops completely
independent, but this will likely slow things down, as
powering is quite expensive (compared to one multiply). Instead we can use the idea
of agglomeration, which means instead of reducing the
code to the finest grain parallel tasks we can, we'll
group some of them into sequential tasks to reduce
overhead. Agglomeration is actually the same principle as the chunking
above, but now we have to think more carefully about
how to split into chunks.
So within each chunk [i,j)
we need to:
- Skip
wn
ahead town^i
- Iterate as before over
[i,j)
Possible factors of K
are easy to choose in this case,
because m
is always a power of two, so K
can be
any power of two less than or equal to m
(including K=1
).
Create a new class based on src/fast_fourier_transform.cpp
, with:
- File name:
src/your_login/fast_fourier_transform_parfor.cpp
- Class name:
hpce::your_login::fast_fourier_transform_parfor
- Display name:
hpce.your_login.fast_fourier_transform_parfor
This class should be based on the sequential version, not on the task based version, so there is only one kind of parallelism.
First apply the loop transformation described above,
without introducing any parallelism, and check it works
with various values of K, via the environment variable
HPCE_FFT_LOOP_K
.
Note that m
gets smaller and smaller as it splits, so
you need to worry about m < K
at the leaves of the
recursion. A simple solution is to use a guarded
version, such that if m < = K
the original code is used,
and if m > K
the new code is used.
Once you have got it working with a non parallel chunked
loop, replace the outer loop with a parallel_for
loop
using simple_partitioner
, and check that it still works
for different values of HPCE_FFT_LOOP_K
. You will
probably not see as much speed-up here, as the dominant
cost tends to be the recursive part.
As before, if HPCE_FFT_LOOP_K
is not set, choose a sensible
default based on your analysis of the scaling with n, and/or
experiments. Though remember, it should be a sensible default
for all machines (even those with 64 cores).
We now have two types of parallelism that we know work,
so the natural choice is to combine them together.
Create a new implementation called fast_fourier_transform_combined
,
using the conventions for naming from before, and integrate
both forms of parallelism. This version should check both
the HPCE_FFT_LOOP_K
and HPCE_FFT_RECURSION_K
variables, and
fall back on a default if either or both is not set.
Task: Create a graph called results/fast_fourier_recursion_versus_iteration.pdf
,
which puts n on the x-axis, time on the y-axis, has four lines:
RECURSION_K=1
andLOOP_K=1
RECURSION_K=1
and the value ofLOOP_K
which seems to work best.LOOP_K=1
and the value ofRECURSION_K
which seems to work best.- The combination of
LOOP_K
andRECURSION_K
which seems to work best.
I'm beeing vague here with "seems to work best". I'll let you resolve it.
Double-check your names all match up, as I'll be trying
to create your transforms both by direct instantiation,
and by pulling them out of the transform registry. Also,
don't forget that "[your_login]" or $LOGIN
does actually mean your
login (your imperial login) needs to be substituted in
wherever it is mentioned.
Specific files (with appropriately named classes) which should exist are:
src/$LOGIN/direct_fourier_transform_parfor_inner.cpp
src/$LOGIN/direct_fourier_transform_parfor_outer.cpp
src/$LOGIN/fast_fourier_transform_parfor.cpp
src/$LOGIN/fast_fourier_transform_taskgroup.cpp
src/$LOGIN/fast_fourier_transform_combined.cpp
Graphs which should exist are:
results/direct_inner_versus_k.pdf
results/direct_outer_time_versus_p.pdf
results/direct_outer_strong_scaling.pdf
results/fast_fourier_time_vs_recursion_k.pdf
results/fast_fourier_recursion_versus_iteration.pdf
However, you can put other files in if you want. Performance results are always interesting, though not required.
Hopefully this should all still be in a git repository, and you will also have a private remote repository in the HPCE organisation. "Push" your local repository to your private remote repository, making sure all the source files have been staged and added. (You can do a push whenever you want as you go (it's actually a good idea), but make sure you do one for "submission"). You may want to do a "clone" into a separate directory to make sure that everything has made it.
After pushing to your private remote repository, zip up your directory, including the .git, but excluding any binary files (executables, objects), and submit it to black-board, just in case.
I would suggest compiling and running your submission in AWS, just to get the feel of it, and to see how it works in a system with lots of cores. A correctly written submission should compile anywhere, with no real dependency on the environment, but it is good to try things out.