Lecture 15 Theory of Ernst & Merchant
L 15.1 Theory of Ernst & Merchant
This story is suggested in 1941 based on the
“principle of minimum energy
consumption”.
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Cutting velocity always remains constant.
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The cutting edge of the tool remains sharp throughout cutting and there is no contact between the workpiece and tool flank.
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There is no sideways flow of chip.
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Only continuous chip is produced.
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There is no built-up Edge.
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No consideration is made of the inertia force of the chip.
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The behaviour of chip is like that of a free-body which is in the state of a stable equilibrium due to the action of two resultant forces which are equal opposite and collinear.
The basis of Ernst and Merchant theory was this suggestion that the shear angle would take up such a value as to reduce the work one in cutting a minimum. For this, is necessary to develop an expression for cutting force in terms of shear angle and then obtain the value of shear angle for which cutting force is a minimum.
From
Fig. 15.1
where
τs = shear strength of the work material on the shear plane
As = area of the shear plane
Ao = cross-sectional area of the uncut chip
τ = mean angle of friction between chip and tool (given by merchant F/ N)
α = working normal rake
From Equation (1) and Equation (2):
Hence
from Equation (3) and Equation (4):
Equation (5) may now be
differentiated with respect to Shear Angle and equated to zero to
find the value of Shear Angle for which Fc is a minimum. The
required value is given by