A cumulative frequency distribution of a random variable x can be represented using the three parameter form of the Weibull equation:
Equation 1
P(x) is the cumulative frequency distribution of a random variable x, in this case either UTS, or
El.TOT
mum allowable value of the analyzed variable, which in this case is 0 for both stress and strain data; θ is the scale param- eter, also referred to as the characteristic value; and m is the shape parameter, also known as the Weibull modulus.
; xo Chill #1, Iteration #2 is the mini-
Equation (1) can be converted into a linear representation by applying the ‘ln’ operator to both sides of the equation to yield the following form:
Equation 2 was made to calculate the slope m in each case.
In this form the equation can be interpreted by the linear form ‘y = mx + b’, where a variable y is plotted in the do- main x to give a line with slope m, and a y-intercept at b. By applying this approach a plot of (y vs. x) was constructed for both the UTS data and the
El.TOT
data sets, and a liner best-fi t
Cross section taken for LOM.
See Figure 4a
►
Chill #1, Iteration #2
Figure 3a. Secondary Dendrite Arm Spacing (λ2
), and porosity measurements on the tensile bar cross-sections from
the Chill #1 (iteration #2) directly below the fracture surface. Cross-section taken is indicated on the fractured surface. Additional Scanning Electron Microscopy / Secondary Electron (SEM/SE) micrographs of the fractured surface were taken as indicated on the fracture surface images (dashed box regions). Included is a high magnifi cation image with a 200 µm bar scale.
International Journal of Metalcasting/Winter 10 35
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