THE BEAM HAS A CIRCULAR CROSSSECTION WHICH IS TAPERED FROM Z
Solution
Let dia at fixed end be d0 and dia at free end where x = L be dl.
At any distance x from fixed end, diameter d = d0 - (x/L)*(d0 - dl)
At distance x, Section modulus Sx = (pi/32) *d3
Sx = (pi/32) [d0 - (x/L)*(d0 - dl)]3
Bending moment at x, Mx = P(L - x)
Bending stress at any cross section = Mx / Sx
= P (L-x) / [(pi/32) [d0 - (x/L)*(d0 - dl)]3]
= (32/pi) P (L-x) / [d0 - (x/L)*(d0 - dl)]3
Putting d0 = 2*2r = 4r and dl = 2*r = 2r, we get
Bending stress = (32/pi) P (L-x) / [4r - (x/L)*(4r - 2r)]3
= (32/pi) P (L-x) / (4r - 2rx/L)3
For max. stress we differentiate it with respect to x and equate it to zero. We get
(-3) (-2r/L) (L-x) (4r - 2rx/L)-4 - (4r - 2rx/L)-3 = 0
(4r - 2rx/L)-3 [(6r/L)(L-x) / (4r - 2rx/L) -1] = 0
Either 4r - 2rx/L = 0 which means x = 2L which is invalid as x can go only to L.
Or (6r/L)(L-x) / (4r - 2rx/L) -1 = 0
(6r/L)(L-x) = 4r - 2rx/L
3 - 3x/L = 2 - x/L
2x/L = 1
x = L/2
