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sm10 120 121

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PROBLEMS (10.120 and 10.121) A simple beam with two different moments of inertia supports
loading as shown in Figs. P10.120 and P10.121.
SOLUTION (10.120)
P
A
EI
3EI
a
a
P/2
M/EI
Pa/2E
A2
B
a
a
C
P/2
x2
A1
Pa/6EI
Pa/3EI
x
x1
A3
x3
y
B
A
vC
θA
x
tC/A = vC
1 Pa
Pa 2
(a) =
2 2 EI
4 EI
2a 5a
1 Pa
Pa 2
(a) =
x2 = a +
A2 =
=
3
3
2 6 EI
12 EI
2
a 3a
Pa
x3 = a + =
A3 =
2 2
6 EI
x1 =
2
a
3
A1 =
(a) θC = 0 from symmetry about C
(b) θC / A = 0 − θ A , θ A = −θC / A , θ C / A = A1 + A2 + A3
Thus,
Pa 2
θ A = − A1 + A2 + A3 = −
(3 + 1 + 2)
12 EI
Pa 2
=
2 EI
Pa 3
vC = tC / A = A1 x1 + A2 x2 + A3 x3 =
(6 + 5 + 9)
36 EI
5 Pa 3
=
↓
9 EI
Continued on next slide
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SOLUTION (10.121)
w
A
EI
wa
B
C
2EI
a
wa
a
M
C
A
x
B
wa2/2
M/EI
4a/3
wa2/EI
2a/3
wa2/2EI
A1
A3
-wa2/2EI
-wa2/4EI
x
A4
Spandrel
parabola
y
A
A2
Spandrel
parabola
3a/4
5a/4
C’’ vC
θA
C
tC/A
C’
tangent at3 A
1 wa 2
1 wa
(a) =
2 EI
2 EI
2
1 wa
wa 3
(a) = −
A3 = −
3 2 EI
6 EI
A1 =
x
B
tB/A
1 wa 2 a
wa 3
( )=
2 EI 2
4 EI
2
1 wa
wa 3
(a ) = −
A4 = −
3 4 EI
12 EI
A2 =
Thus,
4a
2a
5a
3a
) + A2 ( ) + A3 ( ) + A4 ( )
3
3
4
4
3
1
9 wa
θ A = − tB / A = −
2a
32 EI
4
wa
9 wa 4
(32 + 8 − 10 − 3) =
=
48EI
16 EI
t B / A = A1 (
1 wa 3 1 wa 3
−
2 EI 6 3EI
wa 3 9wa 3
5 wa 3
θC = θC / A + θ A =
−
=
3EI 32 EI 96 EI
(a) θC / A = A1 + A3 =
Continued on next slide
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instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other
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a
a
(b) tC / A = A1 ( ) + A3 ( )
3
4
4
4
wa
wa
1 wa 4
=
−
=
6 EI 24 EI 8 EI
1
wa 4 9wa 4
5 wa 4
vC = tC / A − t B / A =
−
=
↓
2
8 EI 32 EI 32 EI
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instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other
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