dingo is a Python package that analyzes metabolic networks.
It relies on high dimensional sampling with Markov Chain Monte Carlo (MCMC)
methods and fast optimization methods to analyze the possible states of a
metabolic network. To perform MCMC sampling, dingo
relies on the C++
library
volesti, which provides
several algorithms for sampling convex polytopes.
dingo
also performs two standard methods to analyze the flux space of a
metabolic network, namely Flux Balance Analysis and Flux Variability Analysis.
dingo
is part of GeomScale project.
To load the submodules that dingo uses, run
git submodule update --init
You will need to download and unzip the Boost library:
wget -O boost_1_76_0.tar.bz2 https://boostorg.jfrog.io/artifactory/main/release/1.76.0/source/boost_1_76_0.tar.bz2
tar xjf boost_1_76_0.tar.bz2
rm boost_1_76_0.tar.bz2
Then, you need to install the dependencies for the PySPQR library; for Debian/Ubuntu Linux, run
apt-get install libsuitesparse-dev
To install the Python dependencies, install Poetry. Then, run
poetry shell
poetry install
To exploit the fast implementations of dingo, you have to install the Gurobi solver. Run
pip3 install -i https://pypi.gurobi.com gurobipy
Then, you will need a license. For more information, we refer to the Gurobi download center.
Now, you can run the unit tests by the following commands:
python3 tests/fba.py
python3 tests/full_dimensional.py
python3 tests/max_ball.py
python3 tests/scaling.py
python3 tests/rounding.py
python3 tests/sampling.py
If you have installed Gurobi successfully, then run
python3 tests/fast_implementation_test.py
You can have a look at our Google Colab notebook
on how to use dingo
.
It quite simple to use dingo in your code. In general, dingo provides two classes:
metabolic_network
represents a metabolic networkpolytope_sampler
can be used to sample from the flux space of a metabolic network or from a general convex polytope.
The following script shows how you could sample steady states of a metabolic network with dingo. To initialize a metabolic network object you have to provide the path to the json
file as those in BiGG dataset or the mat
file (using the matlab
wrapper in folder /ext_data
to modify a standard mat
file of a model as those in BiGG dataset):
from dingo import MetabolicNetwork, PolytopeSampler
model = MetabolicNetwork.from_json('path/to/model_file.json')
sampler = PolytopeSampler(model)
steady_states = sampler.generate_steady_states()
dingo
can also load a model given in .sbml
format using the following command,
model = MetabolicNetwork.from_sbml('path/to/model_file.sbml')
The output variable steady_states
is a numpy
array that contains the steady states of the model column-wise. You could ask from the sampler
for more statistical guarantees on sampling,
steady_states = sampler.generate_steady_states(ess=2000, psrf = True)
The ess
stands for the effective sample size (ESS) (default value is 1000
) and the psrf
is a flag to request an upper bound equal to 1.1 for the value of the potential scale reduction factor of each marginal flux (default option is False
).
You could also ask for parallel MMCS algorithm,
steady_states = sampler.generate_steady_states(ess=2000, psrf = True,
parallel_mmcs = True, num_threads = 2)
The default option is to run the sequential Multiphase Monte Carlo Sampling algorithm (MMCS) algorithm.
Tip: After the first run of MMCS algorithm the polytope stored in object sampler
is usually more rounded than the initial one. Thus, the function generate_steady_states()
becomes more efficient from run to run.
dingo
provides three methods to round a polytope: (i) Bring the polytope to John position by apllying to it the transformation that maps the largest inscribed ellipsoid of the polytope to the unit ball, (ii) Bring the polytope to near-isotropic position by using uniform sampling with Billiard Walk, (iii) Apply to the polytope the transformation that maps the smallest enclosing ellipsoid of a uniform sample from the interior of the polytope to the unit ball.
from dingo import MetabolicNetwork, PolytopeSampler
model = MetabolicNetwork.from_json('path/to/model_file.json')
sampler = PolytopeSampler(model)
A, b, N, N_shift = sampler.get_polytope()
A_rounded, b_rounded, Tr, Tr_shift = sampler.round_polytope(A, b, method="john_postiion")
A_rounded, b_rounded, Tr, Tr_shift = sampler.round_polytope(A, b, method="isotropic_postiion")
A_rounded, b_rounded, Tr, Tr_shift = sampler.round_polytope(A, b, method="min_ellipsoid")
Then, to sample from the rounded polytope, the user has to call the following static method of PolytopeSampler class,
samples = sample_from_polytope(A_rounded, b_rounded)
Last you can map the samples back to steady states,
from dingo import map_samples_to_steady_states
steady_states = map_samples_to_steady_states(samples, N, N_shift, Tr, Tr_shift)
To use any other MCMC sampling method that dingo
provides you can use the following piece of code:
sampler = polytope_sampler(model)
steady_states = sampler.generate_steady_states_no_multiphase() #default parameters (method = 'billiard_walk', n=1000, burn_in=0, thinning=1)
The MCMC methods that dingo (through volesti
library) provides are the following: (i) 'cdhr': Coordinate Directions Hit-and-Run, (ii) 'rdhr': Random Directions Hit-and-Run,
(iii) 'billiard_walk', (iv) 'ball_walk', (v) 'dikin_walk', (vi) 'john_walk', (vii) 'vaidya_walk'.
If you have installed successfully the gurobi
library, dingo turns to the fast mode by default. To set a certain mode you could use the following member functions,
sampler = polytope_sampler(model)
#set fast mode to use gurobi library
sampler.set_fast_mode()
#set slow mode to use scipy functions
sampler.set_slow_mode()
To apply FVA and FBA methods you have to use the class metabolic_network
,
from dingo import MetabolicNetwork
model = MetabolicNetwork.from_json('path/to/model_file.json')
fva_output = model.fva()
min_fluxes = fva_output[0]
max_fluxes = fva_output[1]
max_biomass_flux_vector = fva_output[2]
max_biomass_objective = fva_output[3]
The output of FVA method is tuple that contains numpy
arrays. The vectors min_fluxes
and max_fluxes
contains the minimum and the maximum values of each flux. The vector max_biomass_flux_vector
is the optimal flux vector according to the biomass objective function and max_biomass_objective
is the value of that optimal solution.
To apply FBA method,
fba_output = model.fba()
max_biomass_flux_vector = fba_output[0]
max_biomass_objective = fba_output[1]
while the output vectors are the same with the previous example.
FVA and FBA, restrict the flux space to the set of flux vectors that have an objective value equal to the optimal value of the function. dingo allows for a more relaxed option where you could ask for flux vectors that have an objective value equal to at least a percentage of the optimal value,
model.set_opt_percentage(90)
fva_output = model.fva()
# the same restriction in the flux space holds for the sampler
sampler = polytope_sampler(model)
steady_states = sampler.generate_steady_states()
The default percentage is 100%
.
You could also set an alternative objective function. For example, to maximize the 1st reaction of the model,
n = model.num_of_reactions()
obj_fun = np.zeros(n)
obj_fun[0] = 1
model.biomass_function(obj_fun)
# apply FVA using the new objective function
fva_output = model.fva()
# sample from the flux space by restricting
# the fluxes according to the new objective function
sampler = polytope_sampler(model)
steady_states = sampler.generate_steady_states()
The generated steady states can be used to estimate the marginal density function of each flux. You can plot the histogram using the samples,
from dingo import plot_histogram
model = MetabolicNetwork.from_json('path/to/e_coli_core.json')
sampler = PolytopeSampler(model)
steady_states = sampler.generate_steady_states(ess = 3000)
# plot the histogram for the 14th reaction in e-coli (ACONTa)
reactions = model.reactions
plot_histogram(
steady_states[13],
reactions[13],
n_bins = 60,
)
The default number of bins is 60. dingo uses the package matplotlib
for plotting.
The generated steady states can be used to estimate and plot the copula between two fluxes. You can plot the copula using the samples,
from dingo import plot_copula
model = MetabolicNetwork.from_json('path/to/e_coli_core.json')
sampler = PolytopeSampler(model)
steady_states = sampler.generate_steady_states(ess = 3000)
# plot the copula between the 13th (PPC) and the 14th (ACONTa) reaction in e-coli
reactions = model.reactions
data_flux2=[steady_states[12],reactions[12]]
data_flux1=[steady_states[13],reactions[13]]
plot_copula(data_flux1, data_flux2, n=10)
The default number of cells is 5x5=25. dingo uses the package plotly
for plotting.