The shear stress in a fluid may be expressed as: τα(dvdy)2
where dvdy is the velocity gradient and n is constant. The n value for Newtonian and non- Newtonian fluids will be respectively
A
n=1 and n>1
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B
n<1 and n>1
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C
n=1 and n<1
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D
n=1 and n≠1
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