We report on the a.c. magnetic response of superconducting U P t 3 in a d.c. magnetic field. At low fields (H < H * ), the in-phase susceptibility shows a sharp drop at T c followed by a gradual decrease with decreasing temperature, while the out-of-phase component shows a large peak at T c followed by an unusual broad peak. As the B-C phase line is crossed (H > H * ), however, both the in-phase and out-of-phase susceptibilities resemble the zero-field Meissner curves. These features are only observed for relatively large a.c. excitation fields. We interpret these results in terms of a vortex pinning force which, while comparatively small in the A/B-phases, becomes large enough to effectively prevent vortex motion in the C-phase. PACS numbers 74.70.Tx, 74.25.Ha, 74.60.Ge Typeset using REVT E X 1 Thermal and acoustic transport measurements [1] of the multi-phase heavy fermion superconductor UP t 3 have proven invaluable in deciphering the structure of the zero-field superconducting gap. In particular, the ability of thermal conductivity and ultrasonic attenuation experiments to couple to the excitation spectrum while ignoring the superconducting fraction enables one to measure the momentum space distribution of quasiparticles and thus of the gap itself. Similar studies of the high-field C-phase, however, are greatly complicated by vortex contributions to the electron and phonon scattering rates, and the intrinsic structure and behavior of this phase remain largely unknown. While not usually viewed as such, an a.c. magnetic susceptibility, χ ′ (H dc , T ) + iχ ′′ (T, H dc ), measurement for