Beam_Deflection_Formulae
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BEAM DEFLECTION FORMULAE<br />
BEAM TYPE SLOPE AT FREE END DEFLECTION AT ANY SECTION IN TERMS OF x<br />
1. Cantilever <strong>Beam</strong> – Concentrated load P at the free end<br />
MAXIMUM DEFLECTION<br />
2<br />
Pl<br />
2EI<br />
2<br />
Px<br />
6EI<br />
θ= y = ( 3l−<br />
x)<br />
3<br />
Pl<br />
δ<br />
max<br />
=<br />
3EI<br />
2. Cantilever <strong>Beam</strong> – Concentrated load P at any point<br />
2<br />
Pa<br />
θ=<br />
2EI<br />
3. Cantilever <strong>Beam</strong> – Uniformly distributed load ω (N/m)<br />
2<br />
Px<br />
y = ( 3a− x)<br />
for 0< x<<br />
a<br />
6EI<br />
2<br />
Pa<br />
y = ( 3x− a)<br />
for a< x<<br />
l<br />
6EI<br />
2<br />
Pa<br />
δ<br />
max<br />
= 3 −<br />
6EI<br />
( l a)<br />
3<br />
ωl<br />
6EI<br />
2<br />
ωx<br />
24EI<br />
2 2<br />
θ= y = ( x + 6l − 4lx)<br />
4<br />
ωl<br />
δ<br />
max<br />
=<br />
8EI<br />
4. Cantilever <strong>Beam</strong> – Uniformly varying load: Maximum intensity ω o (N/m)<br />
ω l<br />
24EI<br />
ω x<br />
120lEI<br />
3<br />
2<br />
o<br />
o 3 2 2 3<br />
θ= y = ( 10l − 10l x+ 5lx − x )<br />
4<br />
ωol<br />
δ<br />
max<br />
=<br />
30EI<br />
5. Cantilever <strong>Beam</strong> – Couple moment M at the free end<br />
θ=<br />
Ml<br />
EI<br />
y =<br />
2<br />
Mx<br />
2EI<br />
2<br />
Ml<br />
δ<br />
max<br />
=<br />
2EI
BEAM DEFLECTION FORMULAS<br />
BEAM TYPE SLOPE AT ENDS DEFLECTION AT ANY SECTION IN TERMS OF x MAXIMUM AND CENTER<br />
DEFLECTION<br />
6. <strong>Beam</strong> Simply Supported at Ends – Concentrated load P at the center<br />
2<br />
Pl<br />
θ<br />
1<br />
=θ<br />
2<br />
=<br />
16EI<br />
Px 2<br />
⎛3<br />
l 2 ⎞<br />
y = ⎜ − x ⎟ for 0 < x<<br />
l<br />
12EI<br />
⎝ 4 ⎠<br />
2<br />
3<br />
Pl<br />
δ<br />
max<br />
=<br />
48EI<br />
7. <strong>Beam</strong> Simply Supported at Ends – Concentrated load P at any point<br />
Pbx 2 2 2<br />
2 2<br />
Pb( l − b )<br />
y = ( l −x − b ) for 0 < x<<br />
a<br />
θ<br />
1<br />
=<br />
6lEI<br />
6lEI<br />
Pb ⎡ l<br />
3 2 2 3⎤<br />
Pab(2 l − b)<br />
y = ( x a) ( l b ) x x<br />
θ<br />
2<br />
=<br />
6lEI<br />
⎢<br />
− + − −<br />
⎣b<br />
⎥<br />
⎦<br />
6lEI<br />
for a< x<<br />
l<br />
8. <strong>Beam</strong> Simply Supported at Ends – Uniformly distributed load ω (N/m)<br />
2 2<br />
Pb( l − b ) 32<br />
δ<br />
max<br />
= at x= ( l 2 − b<br />
2<br />
)<br />
3<br />
9 3lEI<br />
Pb<br />
δ= ( 3l<br />
2 −4b<br />
2<br />
) at the center, if a><br />
b<br />
48EI<br />
3<br />
ωl<br />
3 2 3<br />
θ<br />
1<br />
=θ<br />
2<br />
= y = ( l − 2lx + x )<br />
24EI<br />
ωx<br />
24EI<br />
4<br />
5ωl<br />
δ<br />
max<br />
=<br />
384EI<br />
9. <strong>Beam</strong> Simply Supported at Ends – Couple moment M at the right end<br />
θ =<br />
1<br />
θ =<br />
2<br />
Ml<br />
6EI<br />
Ml<br />
3EI<br />
Mlx ⎛ x<br />
y = ⎜1−<br />
6EI<br />
⎝ l<br />
2<br />
2<br />
⎞<br />
⎟<br />
⎠<br />
2<br />
Ml<br />
δ<br />
max<br />
= at x =<br />
9 3EI<br />
2<br />
Ml<br />
δ= at the center<br />
16EI<br />
l<br />
3<br />
10. <strong>Beam</strong> Simply Supported at Ends – Uniformly varying load: Maximum intensity ω o (N/m)<br />
3<br />
7ωol<br />
θ<br />
1<br />
=<br />
360EI<br />
ωox<br />
4 2 2 4<br />
y =<br />
3<br />
( 7l − 10l x + 3x<br />
)<br />
ωol<br />
360lEI<br />
θ<br />
2<br />
=<br />
45EI<br />
ω l<br />
max<br />
0.00652<br />
EI<br />
4<br />
ωol<br />
δ= 0.00651 at the center<br />
EI<br />
4<br />
o<br />
δ = at x = 0.519<br />
l