We have studied the magnetic structure, spin reorientation behaviour and dielectric properties of polycrystalline HoMn1−x
Fe
x
O3 (0.0 ⩽ x ⩽ 0.25) compounds using magnetization, neutron diffraction and dielectric measurements. These compounds crystallize predominantly in the hexagonal phase (P63
cm) with a small phase fraction of the orthorhombic phase (Pnma) which increases with increase in dopant concentration and a total suppression of the hexagonal phase is observed at x = 0.25. Doping Fe at the Mn site leads to an increase in the spin reorientation temperature (T
SR) from 33 K (x = 0) to 55 K (x = 0.1) while the T
N remains nearly constant at 72 K. The magnetic structure of the hexagonal phase was found to be Γ4 (P63′c′m) below T
N and Γ3 (P63′cm′) below T
SR. The magnetic ordering temperature of Ho3+ ions at 2(a) site appears to coincide with the T
SR only in the case of x = 0 sample. The Ho ions at 4(b) site are found to magnetically order below 8 K. The T
N of the Ho ions at both 4(b) and 2(a) sites do not appear to be affected by doping at the Mn site. The temperature variation of the Mn and Ho moments follow the Brillioun function dependence albeit with differing values of the molecular field constant λ
0 and λ
1. Short range magnetic order alone was found for the completely orthorhombic sample (x = 0.25). An anomalous suppression of the dielectric constant (ε) at T
N is observed in the case of hexagonal samples. Further, a linear correlation between Δε (= ε(T) − ε(0)) and the square of the antiferromagnetic moment M, is observed in these compounds.