Hi Edward. I deleted it, since I thought it was a clumsy ugly test.
It only tests: - self.assert_(access(result_dir_name+sep+'resultsR1'+sep+'final'+sep+'phi_ex.out', F_OK)) - self.assert_(access(result_dir_name+sep+'resultsR1'+sep+'final'+sep+'kex.out', F_OK)) - self.assert_(access(result_dir_name+sep+'resultsR1'+sep+'final'+sep+'theta.out', F_OK)) Which can be tested in the other tests. Best Troels 2014-08-19 10:37 GMT+02:00 Edward d'Auvergne <[email protected]>: > Hi Troels, > > Why was this test not necessary? Are all parts already tested in > another test? It's always better to have too much test coverage than > to have small gaps in the coverage. For the test suite, complete > coverage of code paths is always preferable to the total speed of the > test suite. Hence why the test suite takes so long to complete. But > this is why relax is incredibly stable and relatively bug-free. > > Cheers, > > Edward > > > > On 13 August 2014 21:29, <[email protected]> wrote: >> Author: tlinnet >> Date: Wed Aug 13 21:29:57 2014 >> New Revision: 25011 >> >> URL: http://svn.gna.org/viewcvs/relax?rev=25011&view=rev >> Log: >> Deleted systemtest test_r1rho_kjaergaard_man, since it was no necessary. >> >> sr #3135(https://gna.org/support/?3135): Optimisation of the R1 relaxation >> rate for the off-resonance R1rho relaxation dispersion models. >> >> Modified: >> branches/R1_fitting/test_suite/system_tests/relax_disp.py >> >> Modified: branches/R1_fitting/test_suite/system_tests/relax_disp.py >> URL: >> http://svn.gna.org/viewcvs/relax/branches/R1_fitting/test_suite/system_tests/relax_disp.py?rev=25011&r1=25010&r2=25011&view=diff >> ============================================================================== >> --- branches/R1_fitting/test_suite/system_tests/relax_disp.py (original) >> +++ branches/R1_fitting/test_suite/system_tests/relax_disp.py Wed Aug 13 >> 21:29:57 2014 >> @@ -5100,199 +5100,6 @@ >> self.assertAlmostEqual(float(y_prod), >> float(y_comp)) >> >> >> - def test_r1rho_kjaergaard_man(self): >> - """Optimisation of the Kjaergaard et al., 2013 Off-resonance R1rho >> relaxation dispersion experiments using the 'DPL' model. >> - >> - This uses the data from Kjaergaard's paper at U{DOI: >> 10.1021/bi4001062<http://dx.doi.org/10.1021/bi4001062>}. >> - >> - This uses the manual analysis. >> - >> - """ >> - >> - # Cluster residues >> - cluster_ids = [ >> - ":13@N", >> - ":15@N", >> - ":16@N", >> - ":25@N", >> - ":26@N", >> - ":28@N", >> - ":39@N", >> - ":40@N", >> - ":41@N", >> - ":43@N", >> - ":44@N", >> - ":45@N", >> - ":49@N", >> - ":52@N", >> - ":53@N"] >> - >> - >> - # Load the data. >> - self.setup_r1rho_kjaergaard(cluster_ids=cluster_ids) >> - >> - # The grid search size (the number of increments per dimension). >> - GRID_INC = 4 >> - >> - # The number of Monte Carlo simulations to be used for error >> analysis at the end of the analysis. >> - MC_NUM = 3 >> - >> - # Execute the auto-analysis (fast). >> - # Standard parameters are: func_tol = 1e-25, grad_tol = None, >> max_iter = 10000000, >> - OPT_FUNC_TOL = 1e-1 >> - OPT_MAX_ITERATIONS = 1000 >> - >> - result_dir_name = ds.tmpdir >> - >> - # Make all spins free, and select a subset. >> - for curspin in cluster_ids: >> - self.interpreter.relax_disp.cluster('free spins', curspin) >> - # Shut them down >> - self.interpreter.deselect.spin(spin_id=curspin, >> change_all=False) >> - >> - self.interpreter.select.spin(spin_id=':52@N', change_all=False) >> - #self.interpreter.relax_disp.cluster('model_cluster', ':52@N') >> - >> - # Do the analysis manual >> - self.interpreter.spectrum.error_analysis(subset=['46_0_35_0', >> '48_0_35_4', '47_0_35_10', '49_0_35_20', '36_0_39_0', '39_0_39_4', >> '37_0_39_10', '40_0_39_20', '38_0_39_40', '41_0_41_0', '44_0_41_4', >> '42_0_41_10', '45_0_41_20', '43_0_41_40', '31_0_43_0', '34_0_43_4', >> '32_0_43_10', '35_0_43_20', '33_0_43_40', '1_0_46_0', '4_0_46_4', >> '2_0_46_10', '5_0_46_20', '3_0_46_40', '60_0_48_0', '63_0_48_4', >> '61_0_48_10', '62_0_48_14', '64_0_48_20', '11_500_46_0', '14_500_46_4', >> '12_500_46_10', '15_500_46_20', '13_500_46_40', '50_1000_41_0', >> '53_1000_41_4', '51_1000_41_10', '54_1000_41_20', '52_1000_41_40', >> '21_1000_46_0', '24_1000_46_4', '22_1000_46_10', '25_1000_46_20', >> '23_1000_46_40', '65_1000_48_0', '68_1000_48_4', '66_1000_48_10', >> '67_1000_48_14', '69_1000_48_20', '55_2000_41_0', '58_2000_41_4', >> '56_2000_41_10', '59_2000_41_20', '57_2000_41_40', '6_2000_46_0', >> '9_2000_46_4', '7_2000_46_10', '10_2000_46_20', '8_2000_46_40', >> '16_5000_46_0', '19_5000_46_4', '17_5000_46_10', '20_5000_4 6_20', '18_5000_46_40', '26_10000_46_0', '29_10000_46_4', '27_10000_46_10', '30_10000_46_20', '28_10000_46_40']) >> - >> - ##- The 'R2eff' model - >> - self.interpreter.pipe.copy(pipe_from='base pipe', pipe_to='R2eff - >> relax_disp', bundle_to='relax_disp') >> - self.interpreter.pipe.switch(pipe_name='R2eff - relax_disp') >> - self.interpreter.relax_disp.select_model(model='R2eff') >> - self.interpreter.minimise.grid_search(lower=None, upper=None, >> inc=GRID_INC, constraints=True, verbosity=1) >> - >> - self.interpreter.minimise.execute(min_algor='simplex', >> line_search=None, hessian_mod=None, hessian_type=None, >> func_tol=OPT_FUNC_TOL, grad_tol=None, max_iter=OPT_MAX_ITERATIONS, >> constraints=True, scaling=True, verbosity=1) >> - self.interpreter.eliminate(function=None, args=None) >> - self.interpreter.monte_carlo.setup(number=MC_NUM) >> - self.interpreter.monte_carlo.create_data(method='back_calc') >> - self.interpreter.monte_carlo.initial_values() >> - >> - self.interpreter.minimise.execute(min_algor='simplex', >> line_search=None, hessian_mod=None, hessian_type=None, >> func_tol=OPT_FUNC_TOL, grad_tol=None, max_iter=OPT_MAX_ITERATIONS, >> constraints=True, scaling=True, verbosity=1) >> - self.interpreter.eliminate(function=None, args=None) >> - self.interpreter.monte_carlo.error_analysis() >> - >> - # Write results >> - >> #self.interpreter.relax_disp.plot_exp_curves(file='intensities.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', force=True, norm=False) >> - >> #self.interpreter.relax_disp.plot_exp_curves(file='intensities_norm.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', force=True, norm=True) >> - >> #self.interpreter.relax_disp.plot_disp_curves(dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', >> num_points=1000, extend=500.0, force=True) >> - >> #self.interpreter.relax_disp.write_disp_curves(dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', >> force=True) >> - #self.interpreter.value.write(param='r2eff', file='r2eff.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='r2eff', spin_id=None, plot_data='value', file='r2eff.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', force=True, norm=False) >> - #self.interpreter.value.write(param='i0', file='i0.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='i0', spin_id=None, plot_data='value', file='i0.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', force=True, norm=False) >> - #self.interpreter.value.write(param='chi2', file='chi2.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='chi2', spin_id=None, plot_data='value', file='chi2.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', force=True, norm=False) >> - >> - ## Save results as state >> - #self.interpreter.results.write(file='results', >> dir=result_dir_name+sep+'resultsR1'+sep+'R2eff', compress_type=1, force=True) >> - >> - ##- The 'No Rex' model - >> - self.interpreter.pipe.copy(pipe_from='base pipe', pipe_to='No Rex - >> relax_disp', bundle_to='relax_disp') >> - self.interpreter.pipe.switch(pipe_name='No Rex - relax_disp') >> - self.interpreter.relax_disp.select_model(model='No Rex') >> - self.interpreter.value.copy(pipe_from='R2eff - relax_disp', >> pipe_to='No Rex - relax_disp', param='r2eff') >> - self.interpreter.minimise.grid_search(lower=None, upper=None, >> inc=GRID_INC, constraints=True, verbosity=1) >> - >> - self.interpreter.minimise.execute(min_algor='simplex', >> line_search=None, hessian_mod=None, hessian_type=None, >> func_tol=OPT_FUNC_TOL, grad_tol=None, max_iter=OPT_MAX_ITERATIONS, >> constraints=True, scaling=True, verbosity=1) >> - self.interpreter.eliminate(function=None, args=None) >> - >> - ## Write results >> - >> #self.interpreter.relax_disp.plot_disp_curves(dir=result_dir_name+sep+'resultsR1'+sep+'No >> Rex', num_points=1000, extend=500.0, force=True) >> - >> #self.interpreter.relax_disp.write_disp_curves(dir=result_dir_name+sep+'resultsR1'+sep+'No >> Rex', force=True) >> - #self.interpreter.value.write(param='chi2', file='chi2.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'No Rex', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='chi2', spin_id=None, plot_data='value', file='chi2.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'No Rex', force=True, norm=False) >> - >> - ## Save results as state >> - self.interpreter.results.write(file='results', >> dir=result_dir_name+sep+'resultsR1'+sep+'No Rex', compress_type=1, >> force=True) >> - >> - ##- The 'DPL94' model - >> - self.interpreter.pipe.copy(pipe_from='base pipe', pipe_to='DPL94 - >> relax_disp', bundle_to='relax_disp') >> - self.interpreter.pipe.switch(pipe_name='DPL94 - relax_disp') >> - self.interpreter.relax_disp.select_model(model='DPL94') >> - self.interpreter.value.copy(pipe_from='R2eff - relax_disp', >> pipe_to='DPL94 - relax_disp', param='r2eff') >> - self.interpreter.relax_disp.insignificance(level=1.0) >> - self.interpreter.minimise.grid_search(lower=None, upper=None, >> inc=GRID_INC, constraints=True, verbosity=1) >> - >> - self.interpreter.minimise.execute(min_algor='simplex', >> line_search=None, hessian_mod=None, hessian_type=None, >> func_tol=OPT_FUNC_TOL, grad_tol=None, max_iter=OPT_MAX_ITERATIONS, >> constraints=True, scaling=True, verbosity=1) >> - self.interpreter.eliminate(function=None, args=None) >> - >> - ## Write results >> - >> #self.interpreter.relax_disp.plot_disp_curves(dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', >> num_points=1000, extend=500.0, force=True) >> - >> #self.interpreter.relax_disp.write_disp_curves(dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', >> force=True) >> - #self.interpreter.value.write(param='phi_ex', file='phi_ex.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='phi_ex', spin_id=None, plot_data='value', file='phi_ex.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', force=True, norm=False) >> - #self.interpreter.value.write(param='k_AB', file='k_AB.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.value.write(param='kex', file='kex.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.value.write(param='tex', file='tex.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='k_AB', spin_id=None, plot_data='value', file='k_AB.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', force=True, norm=False) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='kex', spin_id=None, plot_data='value', file='kex.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', force=True, norm=False) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='tex', spin_id=None, plot_data='value', file='tex.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', force=True, norm=False) >> - #self.interpreter.value.write(param='chi2', file='chi2.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='chi2', spin_id=None, plot_data='value', file='chi2.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', force=True, norm=False) >> - >> - ## Save results as state >> - #self.interpreter.results.write(file='results', >> dir=result_dir_name+sep+'resultsR1'+sep+'DPL94', compress_type=1, force=True) >> - >> - ##- The 'final' model - >> - self.interpreter.model_selection(method='AIC', modsel_pipe='final - >> relax_disp', bundle='relax_disp', pipes=['No Rex - relax_disp', 'DPL94 - >> relax_disp']) >> - self.interpreter.monte_carlo.setup(number=MC_NUM) >> - self.interpreter.monte_carlo.create_data(method='back_calc') >> - self.interpreter.monte_carlo.initial_values() >> - >> - self.interpreter.minimise.execute(min_algor='simplex', >> line_search=None, hessian_mod=None, hessian_type=None, >> func_tol=OPT_FUNC_TOL, grad_tol=None, max_iter=OPT_MAX_ITERATIONS, >> constraints=True, scaling=True, verbosity=1) >> - self.interpreter.eliminate(function=None, args=None) >> - self.interpreter.monte_carlo.error_analysis() >> - >> - ## Write results >> - >> #self.interpreter.relax_disp.plot_disp_curves(dir=result_dir_name+sep+'resultsR1'+sep+'final', >> num_points=1000, extend=500.0, force=True) >> - >> #self.interpreter.relax_disp.write_disp_curves(dir=result_dir_name+sep+'resultsR1'+sep+'final', >> force=True) >> - #self.interpreter.value.write(param='model', file='model.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.value.write(param='pA', file='pA.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.value.write(param='pB', file='pB.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='pA', spin_id=None, plot_data='value', file='pA.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='pB', spin_id=None, plot_data='value', file='pB.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - self.interpreter.value.write(param='phi_ex', file='phi_ex.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='phi_ex', spin_id=None, plot_data='value', file='phi_ex.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.value.write(param='phi_ex_B', >> file='phi_ex_B.out', dir=result_dir_name+sep+'resultsR1'+sep+'final', >> scaling=1.0, comment=None, bc=False, force=True) >> - #self.interpreter.value.write(param='phi_ex_C', >> file='phi_ex_C.out', dir=result_dir_name+sep+'resultsR1'+sep+'final', >> scaling=1.0, comment=None, bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='phi_ex_B', spin_id=None, plot_data='value', >> file='phi_ex_B.agr', dir=result_dir_name+sep+'resultsR1'+sep+'final', >> force=True, norm=False) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='phi_ex_C', spin_id=None, plot_data='value', >> file='phi_ex_C.agr', dir=result_dir_name+sep+'resultsR1'+sep+'final', >> force=True, norm=False) >> - #self.interpreter.value.write(param='dw', file='dw.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='dw', spin_id=None, plot_data='value', file='dw.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.value.write(param='dwH', file='dwH.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='dwH', spin_id=None, plot_data='value', file='dwH.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.value.write(param='k_AB', file='k_AB.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - self.interpreter.value.write(param='kex', file='kex.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.value.write(param='tex', file='tex.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='k_AB', spin_id=None, plot_data='value', file='k_AB.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='kex', spin_id=None, plot_data='value', file='kex.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='tex', spin_id=None, plot_data='value', file='tex.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.value.write(param='k_AB', file='k_AB.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='k_AB', spin_id=None, plot_data='value', file='k_AB.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.value.write(param='kB', file='kB.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.value.write(param='kC', file='kC.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='kB', spin_id=None, plot_data='value', file='kB.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='kC', spin_id=None, plot_data='value', file='kC.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - #self.interpreter.value.write(param='chi2', file='chi2.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.grace.write(x_data_type='res_num', >> y_data_type='chi2', spin_id=None, plot_data='value', file='chi2.agr', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', force=True, norm=False) >> - >> - # Test of new parameters to write out. >> - self.interpreter.value.write(param='theta', file='theta.out', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', scaling=1.0, comment=None, >> bc=False, force=True) >> - #self.interpreter.value.write(param='theta', file='theta.out', >> dir='~', scaling=1.0, comment=None, bc=False, force=True) >> - #self.assert_(hasattr(cdp.mol[0].res[7].spin[0], 'theta')) >> - >> - ## Save results as state >> - #self.interpreter.results.write(file='results', >> dir=result_dir_name+sep+'resultsR1'+sep+'final', compress_type=1, force=True) >> - ## Save all results in all pipes in state >> - #self.interpreter.state.save(state='final_state', >> dir=result_dir_name+sep+'resultsR1', compress_type=1, force=True) >> - >> - # Assert the file existence of the written value files >> - >> self.assert_(access(result_dir_name+sep+'resultsR1'+sep+'final'+sep+'phi_ex.out', >> F_OK)) >> - >> self.assert_(access(result_dir_name+sep+'resultsR1'+sep+'final'+sep+'kex.out', >> F_OK)) >> - >> self.assert_(access(result_dir_name+sep+'resultsR1'+sep+'final'+sep+'theta.out', >> F_OK)) >> - >> - >> def test_r1rho_kjaergaard_missing_r1(self): >> """Optimisation of the Kjaergaard et al., 2013 Off-resonance R1rho >> relaxation dispersion experiments using the 'DPL' model. >> >> >> >> _______________________________________________ >> relax (http://www.nmr-relax.com) >> >> This is the relax-commits mailing list >> [email protected] >> >> To unsubscribe from this list, get a password >> reminder, or change your subscription options, >> visit the list information page at >> https://mail.gna.org/listinfo/relax-commits > > _______________________________________________ > relax (http://www.nmr-relax.com) > > This is the relax-devel mailing list > [email protected] > > To unsubscribe from this list, get a password > reminder, or change your subscription options, > visit the list information page at > https://mail.gna.org/listinfo/relax-devel _______________________________________________ relax (http://www.nmr-relax.com) This is the relax-devel mailing list [email protected] To unsubscribe from this list, get a password reminder, or change your subscription options, visit the list information page at https://mail.gna.org/listinfo/relax-devel
