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Notch length function

In Fig. 10.12 the dependences of fracture and fracture surface fiactal dimensions, calculated according to the Eqs. (1.9), (4.50), (4.51) and (5.17) and the values D, calculated according to the Eq. (10.17) are adduced as a notch length function for HDPE samples in Sharpy impact tests. The values D and very good correspondence is quite obvious by both the dependence on the course and absolute values. This means, that the fracture energy U value for HDPE is defined by polymer structural state, which is characterized by fractal dimension d. The coupling of U (or A ) with the value d at fracture type (mechanism) correct choice is determined by the dimensions d and d intercommunication, expressed through Poison s ratio value [41]. [Pg.213]

The dependence of these functions (2.a) and (2.b) on the relative notch length for specimens with different fillet radii at the notch base (i.e. sharp cornered and fully rounded) is shown in Fig. 3. [Pg.330]

Where IF is the specimen thickness, a is a the notch length, B is the width of the specimen, S is the distance between the supports, Po is the failure load of a specimen placed without fiber, Z,/is the length of the fiber, df is the diameter of the fiber, Vf is the volume fraction of the fiber, g is the interface parameter, ris fiber/matrix shear stress, and f(a/W) is the shape function calculated as follows Eq.2 ... [Pg.80]

In Fig. 3.3, the comparison of experimental and calculated according to the Eq. (3.10) i values for samples HDPE at different T as a function of sharp notch length a is adduced. As one can see, a good correspondence of experiment and the offered theoretical treatment was received. The value E at T= 293K, obtained by superposition method, is equal to approx. 2.0 GPa, that corresponds well to corresponding values range, obtained in Ref [16]. [Pg.42]

Now the equation for the fracture stress Of estimation as a function of and sharp notch length a can be obtained. In Ref [4], the following definition of stress intensity factor A j as a fimction of was given ... [Pg.175]

FIGURE 17.7 Fracture in tension of a test piece containing a notch or crack, (a) Geometry of the test piece, (b) Energies involved (W) as a function of crack length (L). [Pg.715]

FIGURE 17.9 The effect of the length of a notch L in a test piece on the stress fracture propagation in the piece. Configuration as depicted in Figure 17.7a w is test piece width. The vertical scale is linear and arbitrary. Curve 4 shows the modulus fas a function of L. Meant to illustrate trends. [Pg.721]

In this chapter, the modeling procedures of power line channel have been presented. The deterministic method uses basic network parameters to derive a transfer function of the channel. The investigated deterministic models were determined from an indoor PLC channel. They are specifically topology dependent. For separate network channels, only the cable parameters, the load impedances and the topology of the network are absolutely needed. The LV network is considered as an M nodes and N branches, which is subdivided into several cascaded two-port of small networks. The transfer function of the channel is later obtained by combining easily the T-matrices of the cascades sub networks. The position of notches in frequency response depends on the length of the branched lines. The increase in branched line length tends to limit the available bandwidth in LV channel, but the... [Pg.17]


See other pages where Notch length function is mentioned: [Pg.548]    [Pg.195]    [Pg.196]    [Pg.592]    [Pg.721]    [Pg.330]    [Pg.400]    [Pg.754]    [Pg.548]    [Pg.1334]    [Pg.285]    [Pg.195]    [Pg.401]    [Pg.5]    [Pg.30]    [Pg.184]    [Pg.173]    [Pg.314]    [Pg.330]    [Pg.114]    [Pg.223]    [Pg.38]    [Pg.606]    [Pg.349]    [Pg.582]    [Pg.184]    [Pg.131]    [Pg.132]    [Pg.132]    [Pg.295]    [Pg.319]    [Pg.1367]    [Pg.300]    [Pg.71]    [Pg.160]    [Pg.177]    [Pg.185]    [Pg.316]    [Pg.253]    [Pg.174]    [Pg.425]    [Pg.44]   
See also in sourсe #XX -- [ Pg.213 ]




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