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________________________________________________________________________
PROBLEM (10.108 through 10.111) A cantilever beam is loaded as shown in Figs. P10.108
through P10.111.Determine:
(a) The slope at the free end.
(b) The deflection at the free end.
SOLUTION (10.108)
We have 0
A
θ
= and 0
A
v=.
332
4432
LL
xb== =
13
bh
AEI
=− 2
112 2
339
LwL
EI
=− 3
4
81
wL
EI
=−
(a) Equation (10.48) becomes
0
BA B A
θ
θ
=−=, or
3
4
81
BwL
EI
θ
=
(b) Equation (10.50):
3
45
() ()
3816
BBA LwLL
vt Ax EI
==−+=4
10
243 wL
EI
=
Continued on next slide
M
EI
x
B
v
2
2
9wL
B
θ
A
y
A
2
3
A
R
wL=
x
C
C
w
3
C
B
Parabolic
Spandrel
2
2
9
A
M
wL=2L/3
A
B
Tangent at A
Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or
instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other
reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States
Copyright Act without the permission of the copyright owner is unlawful.
SOLUTION (10.109)
(a) 22
/12
11
24
BBA PL PL
AA EI EI
θθ
==+=− − 2
3
4PL
EI
=
(b) 11 22BBA
vt AxAx== + 22
25
() ()
2346
PL L PL L
EI EI
=− − 3
13
24 PL
EI
=
SOLUTION (10.110)
23
00
1()( )
44 6 24
wL wL
bh
AL
EI EI EI
== =
Continued on next slide
M
EI
x
A
1
1
x
C
2
C
2
A
B
Tangent at A
-PL
P
tC/A
A
2
P
M
EI
x
tB/A
2
x
-PL
A
2
0
A
θ
=
0
A
v
=
M
EI
Cubic
spandrel
A
x
B
L
A
B
Tangent at A
w0L2/6
w0
A
2
0
6
wL
tAB
w0L2/6
0
B
v
=
0
B
θ
=
14
25
n
x
bL
n
+
==
+
Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or
instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other
reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States
Copyright Act without the permission of the copyright owner is unlawful.
(a) 0
/BA B A A
θθθ
=−=, 3
0
24
AwL
EI
θ
=
(b) 3
04
()
24 5
BA A wL L
tvAx EI
== = 4
0
30
wL
EI
=
SOLUTION (10.111)
2
11
2Pa
AEI
=
2
22Pa
AEI
=−
(a) 0
/12BA B A AA
θθθ
=− =
22 2
23
22
BPa Pa Pa
EI EI EI
θ
=− =
(b) /12
34
() ()
23
BA B aa
tvA A
== +
or 22
32 2
() (2)
22 3
BPa a Pa
va
EI EI
=−3
23
12 Pa
EI
=
2
P
a
x
A
1 32a
a
C
a
A
B
Tangent at A
-
P
A
P
a
/
2
M
EI
tB/A
43a
0
0
A
A
v
θ
=
=
A
2
1 / 3 100%

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