The nucleons that can be detected by a neutron monitor at ground level are appreciably absorbed in air [Simpson et al., 1953], making neutron monitor intensity depend exponentially on the amount of air above the monitor. This effect is described by the relation:
dpI=−A·I·dp
where I is the neutron monitor intensity, dpI is the change in I owing to the atmospheric mass change associated with the local air pressure change dp, and A is the neutron monitor mass absorption coefficient. A is positive as defined in equation 1, and its value at ground level is about 0.01 mm Hg−1, or 1% per mm Hg.