When a body is subjected to the two mutually perpendicular stresses, σx & σy, then the center of Mohr’s circle from the origin is

1
\(\frac{{{\sigma _x} + {\sigma _y}}}{2}\)
2
\(\frac{{{\sigma _x} - {\sigma _y}}}{2}\)
3
\(\frac{{2{\sigma _x} + {\sigma _y}}}{2}\)
4
σx + σy

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