Cantilever Beams along a Triangular Load:
Let a cantilever beam loaded with a triangular load as illustrated in Figure
Figure
Consider a section X-X at a distance x from A as illustrated in Figure
Intensity of loading = w/l . x
Moment, M =-(( ½) × (w/l) x × x)(x/3) = - w x3/6l
The governing equation for deflection is following :
EI d 2 y/ dx2 = M = - w x3/6 l
Integrating the eq, we may get
EI (dy/ dx) = - w x4/24 l + C1
EIy=- w x5/120 l + C1 x + C2
The constants C1 and C2 can be found from boundary conditions. The boundary conditions are following :
At B, x = l, dy / dx = 0 ------------- (1)
At B, x = l, y = 0 ------------- (2)
Applying the boundary condition (1) into the Eq. (150), we may get
0 = - wl 3 / 24 + C1
∴ C1 =+ wl 3/ 24
Applying the boundary condition (2) into the Eq. (151), we may get
0 =- wl 4 /120 + wl 4 /24+ C2
∴ C2 =+ wl3 /24
The slope and deflection equations shall be :
EI (dy/ dx) =- w x4/24 l + w l 3/24
EIy =- w x5/120 l + (w l 3 /24 )x - w l 3 / 30
Slope at A, (x = 0),
θA = + wl3 /24 EI
Slope at C (x = l /2),
EI θC = - (w / 24 l )(l/2) 4 + wl 3 /24
= (wl3/24)[-(1/16)+1] = + 15 w l 3 / (24 × 16)
∴ θ C = + 15 wl3 /384 EI
Deflection at A, (x = 0),
y A =- wl 4 /30 EI
Deflection at C, ( x = l/2) ,
EI yC =- wl 4/120 + wl 4/48 - wl 4/ 30
=- wl 4/480 [4 + 10 - 16] =- wl 4/240
∴ yC = wl 4 /240 EI