phase transitions, [17][18][19][20][21][22][23] and it is straightforward to exploit a fragmented BC working body by encapsulating it together with the pressure-transmitting medium. Here we use variable-pressure calorimetry to investigate giant BC effects in the well-known [24,25] MC material MnCoGeB 0.03 near the ≈290 K paramagnetic/hexagonal to ferromagnetic/orthorhombic phase transition (PM/H to FM/O). This transition is associated with a giant change of volume (≈4%) that causes this brittle material to undergo a complete mechanical failure that would be problematic in MC cooling devices. [26] Moderate changes of pressure (|Δp| ≈ 1.7 kbar) drive giant and reversible MC effects of |ΔS| ≈ 30 J K −1 kg −1 and |ΔT| ≈ 10 K. These BC effects are similar to the MC effects that would require impractically large changes of magnetic field (µ 0 ΔH ≈ 10 T) in order to be reversible (µ 0 is the permeability of free space). Our study shows that hydrostatic pressure represents an inexpensive and practical method of driving caloric effects in brittle MC materials. More generally, our study incorporates MnCoGebased compounds into the growing family of multicaloric materials. [27] Above the magnetostructural transition temperature of T 0 ≈ 290 K, MnCoGeB 0.03 adopts the PM/H phase (P63/mmc or Ni 2 In-type space group). [24] On cooling the sample through Hydrostatic pressure represents an inexpensive and practical method of driving caloric effects in brittle magnetocaloric materials, which display first-order magnetostructural phase transitions whose large latent heats are traditionally accessed using applied magnetic fields. Here, moderate changes of hydrostatic pressure are used to drive giant and reversible inverse barocaloric effects near room temperature in the notoriously brittle magnetocaloric material MnCoGeB 0.03 . The barocaloric effects compare favorably with those observed in barocaloric materials that are magnetic. The inevitable fragmentation provides a large surface for heat exchange with pressure-transmitting media, permitting good access to barocaloric effects in cooling devices.