By C. T. Pan, H. Hocheng (auth.), Hong Hocheng, Hung-Yin Tsai (eds.)
Nontraditional machining makes use of thermal, chemical, electric, mechanical and optimum resources of power to bind, shape and lower fabrics. Advanced research of Nontraditional Machining explains in-depth how each one of those complicated machining strategies paintings, their machining approach parts, and approach variables and business purposes, thereby supplying complicated wisdom and clinical perception. This ebook additionally files the most recent and often mentioned study result of a couple of key nonconventional machining procedures for the main involved subject matters in commercial functions, reminiscent of laser machining, electric discharge machining, electropolishing of die and mould, and wafer processing for built-in circuit manufacturing.
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Extra resources for Advanced Analysis of Nontraditional Machining
D) UDcarbon/epoxy, Vfiber ¼ 53 %, D ¼ 4 mm, P ¼ 200 W, t ¼ 8 s. (e) UDcarbon/epoxy, Vfiber ¼ 63 %, D ¼ 2 mm, P ¼ 100 W, t ¼ 8 s. (f) UDcarbon/epoxy, Vfiber ¼ 63 %, D ¼ 2 mm, P ¼ 200 W, t ¼ 8 s. (g) UDcarbon/epoxy, Vfiber ¼ 63 %, D ¼ 4 mm, P ¼ 100 W, t ¼ 8 s. T. Pan and H. (1-89) 2 0 0 15 30 45 60 75 90 Orientation Relative to Fiber Axis (Degree) Fig. 24 (continued) conductivity into FDM schemes, one can predict the HAZ. The comparison between the results of experiment and simulation with constant and temperature-dependent thermal conductivity is shown in Figs.
55). T. Pan and H. 5 [0/90] Glass/PP [0/90] Aramid/PP 0 [0/90] Aramid/PP 0 50 150 100 PQ/V (J/mm) 200 250 Fig. 3 Temperature-Dependent Thermal Conductivity The value of carbon fiber conductivity at temperature exceeding 300 C (573 K) is drastically larger than that at room temperature because of crystallinity . However, the effect of temperature-dependent thermal conductivity was not considered in preceding simulation. The current simulation using constant thermal conductivity shows underpredicted HAZ at higher laser power level and overpredicted HAZ at lower laser power level for both 0 and 90 grooving of Carbon/Epoxy, as shown in Fig.
HAZ seems to remain as long as the workpiece has to be grooved at a certain level of specific laser energy. The existing reference reported that the HAZ is dependent on the laser energy per unit length of grooving (PQ/V) . The simulations of HAZ for grooving UD, Mat, and [0/90] laminates are compared with experimental results. 19 show that HAZ is indeed approximately proportional to the specific laser energy PQ/V. 7). 7, while Carbon/Epoxy has largest ones. Thus, grooving of Aramid/PP produces narrower HAZ.
Advanced Analysis of Nontraditional Machining by C. T. Pan, H. Hocheng (auth.), Hong Hocheng, Hung-Yin Tsai (eds.)