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Structural Theory. Architecture Math Subject.
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IMPORTANT EX'S^ :^ BUILDINGS^ , BRIDGES, O (^) TOWERS (^) (CIIL (^) ENGINEERING)
, PRESSURE VESSELS, MECHANICAL SYSTEMS , AND^ ELECTRICAL SUPPORTING STRUCTURES=IMPORTANT WHEN DESIGNING A (^) STRUCTURE (^) MAKE SURE (^) IT SERVE A^ SPECIFIED FUNCTION FOR PUBLIC^ USE.
STRUCTURAL ELEMENTS-
or TO A^ TENSILE^ FORCE (^). RACING (^) STRUTS)
BEAMS-USUALLY STRAIGHT HORIZONTAL (^) MEM. USED PRIMARILY TO^ CARRY VERTICAL
tO THEIR TOP AND^ BOTTOM. LOAD ·
(^) common (^) buildings Or saschool. · cantilevered =^ ex
CABLES-USUALLY FLEXIBLE^ AND CARRY^ THEIR^ LOADS^ IN^ TENSION.
COLUMNS THAT (^) ARE EITHER (^) PIN OR (^) FIXED CONN
STABILITY r(3m (^) UNSTABLE PERPENDICULAR r3 m STABLE (^) IF REACTIONS/FORCES ARE^ NON-CONCURRENT, ↑
/PARALLEL OR^ SOME^ COMPONENTS^ FORM^ A^ CO-
BX (^08) BX Stable A -- V=^3 M=^2
E 2( Ay UNSTABLE BUT
· UNSTABLE
STRUCTURAL (^) THEORY : ANALYSIS OF^ STRUCTURES 2 DETERMINE^ THE REACTIONS (^) ON THE BEAM (^). 151 M 10KYm ↓ (^) + (^) SOL'Ni ↑ 51/ --^ REG'D : Ax, (^) Ay , Ma *x -^7 5km^ E =^ O; (^2) Fy1 =^0 ; EM = (^0) ;
vvvvvvvv v (^) - (^3) UNIFOR EEX- = (^0) ; MA
[FyT=^0 ; 3
SUPPORT &^ A^ IS^ PIN^ &^ B^ IS^ ROLLER(SMOOTH SURFACE, 500 1b/ft -B vvvvvvvv 4 ft A
" DETERMINE THE HORIZONTAL (^) AND VERTICAL (^) COMPONENTS OF (^) REACTION
FIG.^ 1-32a. uniformly 8 kN^
distributed ↑Xv (^) load zm
=- 2m - i L (^1). 5 m ↓ em- (. )
Diagram) Simplify^ : (^) = - (8kN)(2m) =^
= - In kN/m-GkN/m +^ Bx^ (1. (^5) m) = - (^22) + Bx(1. 5) BX (1.^ 5)^ =^22 Fy](8) BX =^22 j Fx (^) = (^) (s) (^) ti Soln (^) / #B :^ sol'n
2 =^0 ,
3kN At-By- (8)^ = 0
(By] (2m)^ +^ (6^ kN)^ (1m)^ =G
=
[Ft =^ O,
: (^) INDETERMINATE BEAMS.
,
G M X
RA I
RB I
EQUILIBRIUM (^) EQUATIONS : (^2) y =^04 + (^) &Mc = 0 Ra +^ Ri + (^) Rc
36
Ry
-
2 RB(x-^ 12) Fly'
1273
BOUNDARY CONDITIONS^ : 1)8x =^0 , y
( (1) (^) - 2(b)3 +^ 2(12) 6 24RA +^ C =^36
@X = (^24) y
S 0 =^
(12)
2 (18)
+(12)
+, (4) 4 94kx
12Rp
594 ----- (^4) COMBINE 3 & 4 :^ CELIMINATE
, ) COMBINE + ,
, 5
Rx +^ RB + (^) R =^ #S
= 594 2RA +RB =
SUBTRACT s (^) from 4
12Rp = (^558) 96 Ra +^ 12Rg
RA =^2. (^) 625K RB :^30. 75K Rc =^14. 425K 72 Ra (^) + (^) 12 R = 558----
EXAMPLE 2 :^ DETERMINE THE (^) EQUATION OF (^) THE ELASTIC CURVE^.^ El^ IS^ CONSTANT
Condition: 5 ↑ LT M
: O
↑B= Mo Shear
El
El
L = (^0) El = (^) Mo
= (^0) El = MoX +^4 EI^ = Mox+ YtLe &x 2
02 =^0 (IF ASA^ ANG^ SHEAR TUA ANG^ DISPLACEMENT
El = (^) Mox ElE =^ MoX EIV = Mox ? = EXAMPLE 3 :^ THE^ BEAM IS^ SUBJECTED^ TO^ A^ LOAD P
C.^ El^ is^ CONSTANT^ ↓ P A , (^000) B C K 2a^ * a^ A -- - P
EMA =^ ot (^20) = est ↑ ⑪ - ↑ (3a)
za Ay^ = 1 z
INTEGRATION : Fl = M INTERNAL MOMENT^ @^ REGION^ AB^ :
= 0ith
Ay = E ( , (^) )M M (^) = 2 REGION RC^ : 2a1X2[3a X 2 ↓
I-^ 2a - B (^) X
h
3Pa =^ M I 2
DOUBLE INTEGRATION^ : INTEGRATION GOVERNING (^) EQUATION SE^ der-IM dx Ist
Internal moment
Mx +^ C , e Integration Modulus (^) Moment (^) of Inertia-speed or (^) rotation of of Elasticity^ material Equation for (^) truta of
-^ slope characteristic of material of how^ elastic^ itis
EXAMPLE 1 :^ Equation for Displacement Each simply supported^ floor (^) joist shown or deflection. is subjected^ to^ a uniform^ design loading of 4 kN/m^
.^ determine^ the^ maximum deflection of^ the joist
4kN/m 401LN (^) Cutting section ↓ (^) ↓I^ ↓ ↓ r- 5m #I is^ constant^ . &
I
20 ki Ay EM^ c = (^8) t
At
/
: "Ill ,
12m 10kN/m (^) = E10kN/m X^ Im 1
"I
! B = 40 kN (^) dy
1 At T A- (^1 ) 4 12
=
Ma = 480 kN^.^ M^ X = (^) R y = (^0) 3
Fy
Elx = (^) - = Ay-60kN = (^0) Ay = 60kN cut (^) X 10kN/m
=+
M C = 1448 ↑ 60KN EMc =^ of =^ - 60(x) +^ 10x(E) +^ m^ = (^0) EIX =^ Lox- E taxte =- 48x + 5x +^ m^ =^0 M =^ 40 X - 5x2 (^) U 3 1280 El O = (^) 2) -^ E12)"^ + 1440(127^ taz (^8648 4 ) 11280
= 2792 S
#It = x
& BOUNDAry CONDITIONS (^) : Y =^8
= El (^2) 3 #y = -+ X Elo^ = +^4 Cl =^1448 &* E
=+ Y x y = ( ,
Elo (^) = (^) GRE
cut & (^) X My = 450kN/m^ - & (^) X = 0 ↓ 10kN/M = Oft
u6kN
M (^) EF += At^ As (^) - =^ (^1) ( El n #Mc =^ of^ At =^ - = 40(x) +^ 10x(z)^ +M = 0 EN =
(^1440) X +^ =^ -^ 60x + 5x*+ M =^02590 M =^ u0x - 5x
: -