The quaternary structure of proteins determines their biological function, and a majority of proteins exist as oligomers in vivo with miscellaneous architectures. Mass spectrometry (MS) can be applied to study the stoichiometry and interactions of protein complexes by molecular weight measurements under gentle instrumental conditions where noncovalent interactions are preserved in the gas phase. Recently, there have been extensive efforts to also utilize ion mobility (IM) techniques combined with MS for structural studies of noncovalent biological complexes, including virus assembly pathways, because IM provides conformational information, which is not accessible by MS, for these gas-phase ions. Experimentally measured collisional cross sections (CCSs) from IM can serve as constraints for architecture determination by molecular modeling. Additionally, tandem MS can be used to dissociate gas-phase complexes. A protein assembly would ideally dissociate into various noncovalent subcomplexes, and the topology of the original complex could be derived by piecing together all the subcomplex products. The common tandem MS method, collision induced dissociation (CID), involves activation of the complexes by collision with neutral gas atoms or molecules. Typically, CID results in an “asymmetric” dissociation into highly charged monomers and complementary (n 1)-mers (although a few exceptions have been reported), and studies have suggested that unfolding of protein complexes occurs in CID. It is therefore difficult to relate the CCS measurements of CID product ions to the complexes native structure. Tandem MS can alternatively be achieved by surface induced dissociation (SID) where the complexes collide with a surface target. Previous research in our group has shown that several protein complexes dissociate in a more “symmetric” manner with SID than by CID, and have charge distributed more proportionally to the mass. We hypothesized that dissociation might occur in the absence of gradual monomer unfolding for SID because activation by SID is a single-step, higher-energy deposition, fast process that is different from the multistep, slower CID process. SID has recently been applied to determining the quaternary structure of a heterohexameric protein with information from subunit product ions such as heterotrimers unique to SID. We present herein the first IM measurements on the SID products of several protein complexes, along with comparison to CID products, by using a modified quadrupole/IM/time-offlight (Q/IM/TOF) instrument. Briefly, the precursor ions are dissociated by CID or SID cells placed in front of the IM cell. The product ions are subsequently separated based on their size, shape, and charge under the influence of a continuous series of electrical pulses and friction with neutral gas in the IM cell. The drift times of the ions are recorded, with larger and lower-charged ions experiencing longer drift times. Experimental CCSs can be derived from the measured drift times and mass-to-charge-ratios. Theoretical CCSs can be calculated from crystal structures. Nativelike ions should have experimental CCSs similar to the crystal structure, whereas unfolded ions are expected to show larger CCS values because of an increased surface area. We first examined the remaining undissociated pentamer precursor of C-reactive protein (CRP) after activation by either CID or SID. Triethylammonium acetate (TEAA) was added in the electrospraying buffer, which has been reported as a charge reducing additive to increase the stability of protein complexes in the gas phase. Without TEAA no remaining precursor could be observed in SID, even at low acceleration voltages. The addition of TEAA did not cause any remarkable structural change of the protein as the CCSs of the precursor did not change after charge reduction. The + 18 precursor of CRP was selected and activated. Examination of precursor CCSs at various SID acceleration voltages (20–50 V) reveals that most of the CRP pentamer dissociated without extensive increase in CCS of the remaining precursor. In CID, however, the CCS of the undissociated CRP pentamer first decreased at low acceleration voltages and then increased considerably above its dissociation threshold of about 80 V. It reached a stable unfolding intermediate with CID around 100 V, where the CCS does not additionally increase with increasing CID acceleration voltages (data not shown). It is impractical to determine one acceleration voltage at which the amounts of the internal energies deposited in CID and SID are identical because of different mechanisms and complications from the physical properties of large protein complexes. Nonetheless, we show here a representative comparison between CID at 100 V (Figure 1, top right) and SID at 40 V (Figure 1, bottom [*] M. Zhou, Dr. S. Dagan, Prof. V. H. Wysocki Department of Chemistry and Biochemistry, University of Arizona 1306 E. University Blvd., Tucson, AZ (USA) E-mail: vwysocki@email.arizona.edu [] Permanent address: Israel Institute for Biological Research (IIBR) POB 19, Ness Ziona 74100 (Israel)