“…Additionally, continuous grinding on the tooth grooves multiple times blocked the fluid entering the contact area and promoted grinding temperature [18]. According to the grinding temperature model established by Yang et al [19], when a transient point heat source Q d occurred at O(0, 0, 0) in an infinite homogeneous space, as shown in Figure 3, the temperature change at any point M(x, y, z) in the space over time τ could be calculated as: on the tooth grooves multiple times blocked the fluid entering the contact area and promoted grinding temperature [18]. According to the grinding temperature model established by Yang et al [19], when a transient point heat source d Q occurred at (0,0,0) O in an infinite homogeneous space, as shown in Figure 3, the temperature change at any point ( , , ) M x y z in the space over time τ could be calculated as: As shown in Figure 4, when the heat source was replaced by an instantaneous infinitely long linear heat source along the z-axis, and the uniform heat output was s Q , the temperature change to any point ( , , ) M x y z in space over time τ was the integral of the point heat source along an infinitely long straight line, as shown below: In which T was the temperature change, c was the specific heat capacity of workpiece material, ρ was the density of workpiece material, and α was the thermal conductivity.…”