Lots of help from Cristian Botez, Ashfia Huq, Yuan-Hon Kiang, Silvina Pagola, many other people who don’t care to be mentioned.

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Presentation transcript:

Lots of help from Cristian Botez, Ashfia Huq, Yuan-Hon Kiang, Silvina Pagola, many other people who don’t care to be mentioned. Use of Synchrotron Radiation to Study Polymorphs of Pharmaceuticals

Why powders? Why synchrotron radiation? Examples: Real problem - distinguishing polymorphs with similar x-ray patterns Real problem – determining small concentrations of a protected polymorph Crystal structure solutions Proxy for a real problem – determining solid form of a small amount of API in a finished tablet How synchrotron radiation?

Single crystal diffraction is regarded as the gold standard for structure determination. (With ~100  m single crystal, structure determination is “routine”.) -but- Determination of a crystal structure is only a subset of the structural information generally desired. IN THE CONTEXT OF POLYMORPHISM Many materials first show up as powders. Many materials are available only as powders. Measurements of solid mixtures are important, even independent of the crystal structure.

Incident beam x-rays or neutrons Sample (111) (200) (220) Real Space - Debye-Scherrer cones Typically grains of 1  m (10 9 molecules) each, packed to 50% density

Where does a powder diffraction pattern come from? Instrument – Is your instrument aligned correctly? (Can you index simple patterns such as lactose hydrate) Are relative intensities measured accurately? (Preferred orientation, illuminated volume, …) Strong pitch for use of synchrotron radiation (Not giving an unbiased comparison of available instruments) Three levels of understanding of a powder diffraction pattern 1.Collection of peaks (fingerprint) 2.PROFILE FIT. Use known lattice (or determine lattice) to constrain all peak positions. Instead of ~20 peak positions, you have 1 to 6 lattice parameters. Intensitites are matched to the data. 3.RIETVELD FIT. Use known structure (or solve structure). Intensitites determined by crystal structure.

What’s in your pill? (fake) Data taken with very good (~0.007 º FWHM) resolution at NSLS Example 1

A little work turns up this entry in the Powder Diffraction File

What are these weak peaks? The active ingredient?

Lattice parameters -> possible peak positions Space group -> some of those peak positions are not seen Positions of atoms within the unit cell -> relative intensities of peaks within each phase X-ray diffractometer optics -> lineshape parameters (fundamental parameters on well-characterized instrument) Crystallite size, internal strain, lattice defects -> lineshape parameters (not usually very interesting; adjust parameters to give a good fit to lineshape data) Rietveld method: look at all of your data. Compare the profile with a model, not just the intensities of the diffraction peaks.

Not the best fit in the world, but clear enough “Missing” peaks are actually from lactose monohydrate, not in PDF!

Anode Electrons, 50 keV 40 mA X-ray tube Bragg-Brentano Focus diverging beam. Moderate resolution, sensitive to sample displacement, transparency Debye-Scherrer Resolution limited by divergence, parallax

Magnetic Field Electrons, 2.8 GeV = 5500 mc mA % of c 1/  ~ 0.01  Synchrotron Radiation X-ray brightness Photons/time/solid angle/bandwidth 10 5 (This is NOT an x-ray laser)

The sample geometry can have a profound influence on the measured intensity. Preferred orientation. There are various means to minimize issues of preferred orientation. It is usually best to load samples in a thin glass tube. (Not a perfect guarantee.) Bragg-Brentano Broad beam Measure angle, not position

Powder diffraction station at X3B1 beamline, National Synchrotron Light Source, Brookhaven National Laboratory, U. S. A. (available for general users, rent, or collaboration) Ion chambersample GE (111) analyzer crystal Scintillation detector Parallel, Monochromatic X-ray beam Si(111) double monochromator From storage ring

Form I Form II Lab(Sealed Tube) and Synchrotron XRD patterns of Enalapril Maleate 22 =1.15Å, 2  Cu K  1 Form I Form II

Advantages of Synchrotron Radiation for Powder Diffraction Intensity Sharper peaks Distinguish nearby peaks and locate peaks more precisely Better Signal to Background (see weak peaks close to strong ones) For analyzer crystal setup, the resolution does not degrade with sample size (intact samples) For analyzer crystal setup, the resolution does not degrade with shorter wavelength. Freedom from parallax errors due to alignment, transparency Generally easier to use environmental chambers. (Tunability can tailor x-ray penetration to the problem at hand, make use of anomalous dispersion.)

Examples of identification of polymorphs with synchrotron radiation data

This drug product has two polymorphs that can’t be quantified except by Rietveld. Compare lab vs. synchrotron data sets.

Two polymorphs of Zantac®, ranitidine hydrochloride

Structure Solution from powder data. (PS & Silvina Pagola, Nature 404, 647 (2000); ACA Transactions (2002); several papers in preparation) PSSP is open source, simulated annealing software. Three examples: 2½ polymorphs of 4’ methyl ROY Form II ranitidine hycrochloride (interesting challenge for sim. annealing) Form II enalapril maleate previously unknown structure Malaria pigment  hematin,  -D-Mannitol anhydride, R(-)-Albuterol sulfate, 2-Hydroxy-N-[3(5)-Pyrazolyl]-1,4-napthoquinone-4-imine, N-(p-tolyl)-dodecylsulfonamide, …

Pigments from Xiaorong He and coworkers in Byrn’s group at Purdue, Dept. of Pharmacy 4 polymorphs of the same molecule - different colors. 1 solved by single crystal diffraction at Purdue 2 solved by S. Pagola from powder data We’re still working on one. CH 3 N NO 2 NC CH 3 H S orange red dark red light red

orange dark red Comparison of powder vs. single crystal solution of DR

Ranitidine hydrochloride form II Undertake a project like this with very good data

Space Group : P 2 1 /n 6 Spatial coordinates : position 3 Eulerian angles : orientation 11 Torsions. 20 parameters Ranitidine HCl (Zantac®) is a very widely used drug for ulcers, excess production of stomach acid. There is an interesting subtlety in its crystal structure. Monoclinic, Z=4 a=18.808Å, b=12.981Å, c=7.211Å  =95.057°,

Two candidate solutions from PSSP Two others All four, superimposed. Disorder, or inability of powder data to distinguish a few of the atoms?

Atomic structure of our best Rietveld refinement of a single molecule. Essentially independent of which solution we start from. R wp = 11.12%,  2 = 10.56

R wp = 8.43%,  2 = 4.51

Refinement incorporating disorder. 50% occupancy of each of two sites for N14, C16, C18, O20, and O21. R wp =8.39%,  2 = 4.51 All thermal parameters independently refined! Gentle restraints on bond lengths. This is clearly the correct solution, which includes molecular disorder.

The answer, including disorder, was already known from single crystal experiment. T. Ishida, Y. In, M. Inoue (1990)

The crystallographic problem: 1.Single crystals, small molecules: # of observations >> # of atoms  Demand reasonable atomic distances, angles, etc. 2.Proteins (single crystals, data with resolution ~ 2–3 Å ):  Use sequence data, strong constraints on amino acid structure. 3.Structures determined from powders by direct methods, etc.:  Demand reasonable atomic distances, angles, etc. Structures from powders using direct space: models of known molecular structure  Caution: many bond distances and angles are built in, so there is less redundancy. No rigorous argument that any solution we find is correct. We look for heuristic consistency checks, generally based on getting a “reasonable” solution, and having redundant data.

Conclusions for Ranitidine HCl In this case, the crystal structure contains subtleties not expected in the starting model. Careful monitoring of the progress of the refinement shows trouble if you ignore the disorder that is suggesting itself through nonsense thermal parameters. Careful monitoring of the simulated annealing steps even show that the correct answer is knocking at the door, even though it was not originally invited.

Enalapril Maleate is a potent angiotensin converting enzyme (ACE) inhibitor with two known polymorphs, Form I and Form II. The single crystal structure of Form I has been known for almost twenty years. On the other hand, the crystal structure of Form II has never been reported before because of the difficulty to obtain single crystals of this polymorph, which is made by water slurry of Form I. The crystal structure of Form II is of interest for several reasons: 1. Form II is the more stable of the two polymorphs. 2. The two forms are structurally similar based on X-ray, IR, and solid-state NMR. 3. The conformation of ACE inhibitors is important to their biological activity.

LeBail Refinement Cell indexed using 25 peaks in ITO Index measured pattern and extract intensities Orthorhombic P a= b=6.642 c=11.210

a= b=6.640 c=  form I a= b=6.642 c= form II No Solution from simulated annealing methods Powder Solve Crashed PSSP : ran for  time without success DASH – we haven’t tried it yet. 23 parameters: 11 enalapril torsions (+2 maleate) + 12 orientation + position Enalapril Maleate Monoclinic P2 1 /c Orthorhombic P

Form I Form II green:carbon yellow:nitrogen red:oxygen

Real business problem: _____ has a patented polymorph of _____, and suspects that _____ is selling material that infringes. It is desired to examine the commercial tablets and determine the polymorph of the API for potential litigation. Proxy: Examine commercial tablet of Endocet 500/7.5 Gross tablet 607 mg Acetaminophen 500 mg – known lattice & structure Oxycodone (as HCl) 7.5 mg – pattern in PDF but lattice unknown,* * In general, I’d like to get better info into the PDF database. Please get in touch if you can help.

Powder patterns of oxycodone hydrochloride from ICDD Powder Diffraction File. Strucutures and lattices are not known.

There are five synchrotron x-ray sources in the US suitable for experiments like these. ~40 worldwide. In my humble opinion, the most usable is NSLS at Brookhaven Lab users per year, of whom ~30% are new. All of these facilities have active programs to serve the interests of people who want to use them. Modes of access: Write a proposal, wait several months, no charge for x- rays, publish results. Pay ~$300 - $5000/hr for time used, you own the data, get access within hours to weeks.

What is the real difference between working at a synchrotron radiation source vs. with a laboratory x-ray diffractometer?

Acknowledgements : Ashfia Huq, Silvina Pagola (now at Apotex) Dept. of Physics & Astronomy, SUNY Stony Brook, Y.-H. Kiang, Wei Xu Pharmaceutical Research, Merck & Co., Inc. West Point, PA, “Anonymous” referees who goaded us into completing the Ranitidine story. Advertisements: Workshop on Frontiers of Powder Diffraction at the NSLS user meeting, May 19. nslsweb.nsls.bnl.gov. The International Centre for Diffraction Data is planning to run its third Pharmaceutical Powder X-ray Diffraction Symposium in See me to get on the mailing list, or browse References : Ashfia Huq and P.W. Stephens, “Subtleties in Crystal Structure solution from powder diffraction data using Simulated Annealing Method”, J. Pharm Sci Y.-H. Kiang, Ashfia Huq, Peter W. Stephens, Wei Xu, “Structure Determination of Enalapril Maleate Form II from High-Resolution X-ray Powder Diffraction Data,” submitted to Journal Pharm. Sci. Pagola S. and P.W.Stephens, Mater. Sci. Forum 2000, 321, 40 (Source code and documentation for PSSP are available at

Conclusions: Think about x-ray diffraction as giving information about the fundamental structure of your material, not just a list of peaks. This is a data-driven enterprise. High quality data is very important. I do not want to leave the impression that synchrotron radiation is prerequisite to good data. Nor that SR is guaranteed to provide an important breakthrough. It certainly helps. Research carried out in part at the National Synchrotron Light Source at Brookhaven National Laboratory, which is supported by the US Department of Energy, Division of Materials Sciences and Division of Chemical Sciences. The SUNY X3 beamline at NSLS is supported by the Division of Basic Energy Sciences of the US Department of Energy under Grant No. DE-FG02-86ER45231.