Fig。 8。 The relationship of the steady stress with respect to the temperature and the strain rate, respectively: (a) the relationship between lns and lnε_; (b) the relationship between s and lnε_; (c) the relationship between ln½sinhðαsÞ] and lnε_ and (d) the relationship between ln½sinhðαsÞ] and T−1。
combining the values of n and β, namely α ¼ β=n ¼ 1:24~ 10−2 MPa−1 。
To obtain the value of Q , the natural logarithm of Eq。 (1) results in the following equation:
lnε_ ¼ ln A þ nln。sinhðαsÞ。− RT ð6Þ
Based on Eq。 (6), the value of n is modified as the linear proportion factor of lnε_ with respect to ln½sinhðαsÞ]。 The value of n is determined as 4。906 according to the average value of slope of the lines at all the different deformation temperatures as shown in Fig。 8(c)。
For the given strain rates, differentiating T −1 in Eq。 (6) results in
Eq。 (7)
。 ∂ln½sinhðαsÞ 。
Fig。 9。 The relationship between ln½sinhðαsÞ] and lnZ。
Q ¼ nR
∂T −1 ε_
ð7Þ
follows:
7
4:906 3
The value of Q can be calculated as 101。3 ~ 103 J mol−1 by
ε_ ¼ 1:48 ~ 10 ½sinhð0:0124sÞ]
~ expð−101:3 ~ 10 =RT Þ ð10Þ
combining the values of n and R with the average value of slope of all the lines at the different strain rates as shown in Fig。 8(d)。
In general, the Zener–Hollomon parameter Z can be used to describe the comprehensive influence of the strain rate and the temperature on the flow stress of the metal materials during hot
The substitution of Eq。 (10) into Eq。 (8) leads to
Z ¼ ε_expðQ =RT Þ¼ 1:48 ~ 107 ½sinhð0:0124sÞ]4:906 ð11Þ
According to Eq。 (8), the following formulation can be obtained:
。Z。1=n
deformation [29]。
n
sinhðαsÞ¼ A
ð12Þ
Z ¼ ε_expðQ =RT Þ¼ A½sinhðαsÞ]
The natural logarithm of Eq。 (8) results in
According to the definition of the hyperbolic sinhðαsÞ, Eq。 (12) can be transformed into the following expression:
ln Z ¼ ln A þ nln½sinhðαsÞ] ð9Þ
According to Eq。 (9), the value of lnA is the intercept of the
expðαsÞ−1 ¼ 0 ð13Þ
fitting line of lnZ with respect to ln½sinhðαsÞ] in the lnZ coordinate axis as shown in Fig。 9, so the value of A is further determined as
Eq。 (13) can be further expressed as follows:
1:48 ~ 107 s−1 。
1 2。Z。1=n
sffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi 3
。Z。
By substituting the values of A, α, nand Q into Eq。 (1), the constitutive equation of 7A09 aluminum alloy is expressed as 复杂铝合金圆盘的等温精密锻造英文文献和中文翻译(6):http://www.youerw.com/fanyi/lunwen_96941.html