Typically, the force between paramagnetic particles in a uniform magnetic field is calculated using either dipole-based models or the Maxwell stress tensor combined with Laplace's equation for magnetostatics. Dipolebased models are fast but involve many assumptions, leading to inaccuracies in determining forces for clusters of particles. The Maxwell stress tensor yields an exact force calculation, but solving Laplace's equation is very time consuming. Here, we present a more elaborate dipole-based model: the micro-mutual-dipolar model. Our model has a time complexity that is similar to that of other dipole-based models but is much more accurate especially when used to calculate the force of small aggregates. Using this model, we calculate the force between two paramagnetic spheres in a uniform magnetic field and a circular rotational magnetic field and compare our results with those of other models. The forces for three-particle and ten-particle systems dispersed in two-dimensional (2D) space are examined using the same model. We also apply this model to calculate the force between two paramagnetic disks dispersed in 2D space. The micro-mutual-dipolar model is demonstrated to be useful for force calculations in dynamic simulations of small clusters of particles for which both accuracy and efficiency are desirable. [5,6], biomedical sensing [7,8], propulsion and transportation in fluids [9,10], and force probes [11,12]. In these applications, the magnetic force between paramagnetic particles must be calculated accurately. Typically, dipole-based models, such as the dipolar model (DM) and the mutual-dipolar model (MDM), are used to calculate the force between paramagnetic particles placed in an external magnetic field [2,5,13]. Dipole-based models are usually fast but inaccurate for systems in which particles are close to one another. Such models are inaccurate because they do not consider multipolar effects [14]. The exact force can be calculated by solving a Laplace equation for magnetostatics with multiple boundary and initial conditions and calculating the Maxwell stress tensor for each particle [15]. The solution to the Laplace equation can be analytically approximated by a solid harmonics expansion with the Hobson formula applied to unify the coordinate system [14,16]. This coordinate unification is very computationally expensive and suffers from singularity-related issues [17,18]. A numerical solution to Laplace's equation can be obtained by using a smoothed representation of susceptibility to replace the boundary conditions [17]; this method is referred to as the Laplace equation solver (LES) method. This numerical approach is stable in terms of error propagation but still computationally time consuming.Here, we present a more-sophisticated dipole-based model that considers mutual interactions between dipole moments and multipolar effects. All dipole-based models are based on the fact that a single spherical paramagnetic particle is uniformly magnetized in the presence of a uniform magnetic * Correspondin...