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Structural Theory Notes, Study notes of Theory of Structures

Structural Theory. Architecture Math Subject.

Typology: Study notes

2022/2023

Uploaded on 05/28/2025

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STRUCTURE
-
REFERS
TO
A
SYSTEM
OF
CONNECTED
PARTS
USED
TO
SUPPORT
ALOAD
.
IMPORTANT
EX'S
:
BUILDINGS
,
BRIDGES
,
O
TOWERS
(CIIL
ENGINEERING)
SHIP
AND
AIRCRAFT
FRAMES
,
TANIS
,
PRESSURE
VESSELS
,
MECHANICAL
SYSTEMS
,
AND
ELECTRICAL
SUPPORTING
STRUCTURES
=IMPORTANT
WHEN
DESIGNING
A
STRUCTURE
MAKE
SURE
IT
SERVE
A
SPECIFIED
FUNCTION
FOR
PUBLIC
USE
.
-
ENGR
.
MUST
TAKE
ACCOUNT
SAFETY
,
AESTHETICS
&
SERVICEABILITY
,
WHILE
TAKING
INTO
CONSIDE-
RATION
ECONOMIC
AND
ENVIRONMENTAL
CON-
STRAINTS
.
-
STRUCTURAL
ELEMENTS
-
TIE
RODS-STRUCTURAL
MEMBERS
SUBJECTED
or
TO
A
TENSILE
FORCE
.
BRACING
STRUTS)
pf3
pf4
pf5
pf8
pf9
pfa
pfd
pfe
pff
pf12
pf13
pf14
pf15
pf16
pf17
pf18
pf19
pf1a

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STRUCTURE

  • REFERS TO A (^) SYSTEM OF (^) CONNECTED PARTS USED (^) TO

SUPPORT

ALOAD.

IMPORTANT EX'S^ :^ BUILDINGS^ , BRIDGES, O (^) TOWERS (^) (CIIL (^) ENGINEERING)

SHIP AND AIRCRAFT FRAMES, TANIS

, PRESSURE VESSELS, MECHANICAL SYSTEMS , AND^ ELECTRICAL SUPPORTING STRUCTURES=IMPORTANT WHEN DESIGNING A (^) STRUCTURE (^) MAKE SURE (^) IT SERVE A^ SPECIFIED FUNCTION FOR PUBLIC^ USE.

  • (^) ENGR (^). MUST TAKE ACCOUNT SAFETY , AESTHETICS & (^) SERVICEABILITY , WHILE^ TAKING^ INTO^ CONSIDE- RATION ECONOMIC^ AND^ ENVIRONMENTAL^ CON- STRAINTS.

STRUCTURAL ELEMENTS-

TIE RODS-STRUCTURAL MEMBERS SUBJECTED

or TO A^ TENSILE^ FORCE (^). RACING (^) STRUTS)

BEAMS-USUALLY STRAIGHT HORIZONTAL (^) MEM. USED PRIMARILY TO^ CARRY VERTICAL

LOADS.

=> BEAM CROSS^ SECTIONS^ MAY ALSO^ BE^ "BUILT^ UP"^ BY^ ADDING^ PLATES

tO THEIR TOP AND^ BOTTOM. LOAD ·

simply ,^ fixed^ ,^ continuous^

  • (^) common (^) buildings Or saschool. · cantilevered =^ ex

: Overhang

CABLES-USUALLY FLEXIBLE^ AND CARRY^ THEIR^ LOADS^ IN^ TENSION.

CABLE-TENSION
ARCHES-COMPRESSION
FRAMES-OFTEN USED^ IN^ BUILDINGS^ AND^ ARE^ COMPOSED^ OF^ BEAMS^ &

COLUMNS THAT (^) ARE EITHER (^) PIN OR (^) FIXED CONN

  • ECTED.
INDETERMINATE
  • "UNKNOWN VALUE "
  • DILI MASOLVE SURFACE STRUCTURES^
  • made from material having a small thickness^ compared
to its^ dimensions

STABILITY r(3m (^) UNSTABLE PERPENDICULAR r3 m STABLE (^) IF REACTIONS/FORCES ARE^ NON-CONCURRENT, ↑

UNSTABLE IF^ MEMBER REACTIONS ARE CONCURRENT

/PARALLEL OR^ SOME^ COMPONENTS^ FORM^ A^ CO-

LLAPSIBLE MECHANISM.

EX :

BX (^08) BX Stable A -- V=^3 M=^2

E 2( Ay UNSTABLE BUT

THROUGH

INSPECTION ITS STABLE

· UNSTABLE

  • I F

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) ;

A /

vvvvvvvv v (^) - (^3) UNIFOR EEX- = (^0) ; MA

AyT 12 In^ Ax =^ 0 kN

[FyT=^0 ; 3

DETERMINE THE^ REACTIONS ON^ THE BEAM . ASSUME

SUPPORT &^ A^ IS^ PIN^ &^ B^ IS^ ROLLER(SMOOTH SURFACE, 500 1b/ft -B vvvvvvvv 4 ft A

7ft 3ft

PROBLEM 3 :^ STRUCTURAL THEORY

" DETERMINE THE HORIZONTAL (^) AND VERTICAL (^) COMPONENTS OF (^) REACTION

AT THE PINS A , B, AND C Of THE TWO MEMBER FRAME SHOWN IN

FIG.^ 1-32a. uniformly 8 kN^

3kN/m &

distributed ↑Xv (^) load zm

M

=- 2m - i L (^1). 5 m ↓ em- (. )

FBD :^ (Free^ Body

Diagram) Simplify^ : (^) = - (8kN)(2m) =^

  • 16kNm = - -kn(2m) =-^6 knm

= - 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

Em

= 0 , ↑ y^ =^3

2 =^0 ,

3kN At-By- (8)^ = 0

(By] (2m)^ +^ (6^ kN)^ (1m)^ =G

Rea =- 3kN-E

=

3 kN

[Ft =^ O,

  • (^) By -^ 6kN +^6 =^0 Ex -^ 3kN EEEKN

SAMPLE PROBLEM

: (^) INDETERMINATE BEAMS.

DETERMINE THE^ REACTIONS ATTHE SUPPORTS A , B , AND C^

,

THEN DRAW^ THE^ SHEAR^ AND^ MOMENT^ DIAGRAMS.^ El^ IS^ CONSTANT

G M X

SOLUTION :

RA I

X

RB I

RC

EQUILIBRIUM (^) EQUATIONS : (^2) y =^04 + (^) &Mc = 0 Ra +^ Ri + (^) Rc

  • 12 - [3(127] =^0 - Ra(24) - R (^) +(12) + (^) + 2 (18) +^ [3(1)7( Ra (^) + (^) RB + Rc =^48 .... (^) " 22A

Ry

36

M = Rxx +^ Ry(X

12(x

      • [3(
      • 127] · (XR) 2

M =

Ry

  • (^) + (^) RB(x
     - 

m(x

      • (^) (x-

2 RB(x-^ 12) Fly'

  • (^) b(x- a )
  • (x

1273

  • (^4) 2 2 3 Fly =
  • 1)" - 2(x - 3) - t(x - 12)4 +^ c^ , x (^) + 2

BOUNDARY CONDITIONS^ : 1)8x =^0 , y

  1. ex = 12 , y = 0 C

( (1) (^) - 2(b)3 +^ 2(12) 6 24RA +^ C =^36

  • (^) ... 3

@X = (^24) y

S 0 =^

Rx(24)

(12)

2 (18)

+(12)

+, (4) 4 94kx

12Rp

c

594 ----- (^4) COMBINE 3 & 4 :^ CELIMINATE

C

, ) COMBINE + ,

, 5

⑨ 24RA^

+ 4 =^36

Rx +^ RB + (^) R =^ #S

96 Ry^ HERBEC

= 594 2RA +RB =

SUBTRACT s (^) from 4

: 72RA^ +

12Rp = (^558) 96 Ra +^ 12Rg

  • 2 =^594

24RA +^ c =^36

RA =^2. (^) 625K RB :^30. 75K Rc =^14. 425K 72 Ra (^) + (^) 12 R = 558----

DOUBLE INTEGRATION^ METHOD

EXAMPLE 2 :^ DETERMINE THE (^) EQUATION OF (^) THE ELASTIC CURVE^.^ El^ IS^ CONSTANT

  • Ji & L^ X FBB (^7) * ↑ Mo M (^) & L (^) ↑ EMp^ = Ot By (^) Mp-Mo = 0

MB =^ Mo

Cut &X:

Boundary

Condition: 5 ↑ LT M

& x^0

: O

"Slope

↑B= Mo Shear

Internal

El

= Mox +

El

= M

L = (^0) El = (^) Mo

& x =^0 , V

= (^0) El = MoX +^4 EI^ = Mox+ YtLe &x 2

El X^ =^ Mox+^ C, x^ +^ Ce

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

AT ITS^ END.^ DETERMINE^ THE^ DISPLACEMENT @

C.^ El^ is^ CONSTANT^ ↓ P A , (^000) B C K 2a^ * a^ A -- - P

  • i - X X, *

A

  • Y

A

EMA =^ ot (^20) = est ↑ ⑪ - ↑ (3a)

  • By (2a) =^0 Ay +^24 -^ p =^0 2 By = (^) P(39) (^) = By

Ay (^) +^0

za Ay^ = 1 z

INTEGRATION : Fl = M INTERNAL MOMENT^ @^ REGION^ AB^ :

OLX, 12a^

EMec

= 0ith

  • X^ =

Ay = E ( , (^) )M M (^) = 2 REGION RC^ : 2a1X2[3a X 2 ↓

I-^ 2a - B (^) X

  • za 34) Me I EMy

h

  • (xc)^
    • (x2-2a) - M
= O

# -^ exe^ -

3Pa =^ M I 2

  • 3 EM! P (^) X 2

DOUBLE INTEGRATION^ : INTEGRATION GOVERNING (^) EQUATION SE^ der-IM dx Ist

#M-

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

#tuxtre

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

  • C A B (^) Ax

I

= zi--^ em--1By^

20 ki Ay EM^ c = (^8) t

= 0 va

At

/

20kN/m

INTEGRATION

: "Ill ,

  • #^ A = M ~ A B 12 m nam #^ = 60x
  • 5x =&M (^) 601N
LE12mt =^

12m 10kN/m (^) = E10kN/m X^ Im 1

120kN - 5x

"I

+ &d^
  • ↓d^ = E

&Y^

    • 4 (

! B = 40 kN (^) dy

1 At T A- (^1 ) 4 12

El

=

  • taxte A+ 24580kN^ . m] EN = (^) - BOUNDARY^ CONDITIONS = 60kN(8m]^
+ M^ =^0 X =^ R^
- =^0

Ma = 480 kN^.^ M^ X = (^) R y = (^0) 3

E

Fy

= 0 +^1

Elx = (^) - = Ay-60kN = (^0) Ay = 60kN cut (^) X 10kN/m

Elo

=+

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

Ch

= 2792 S

#It = x

    • 1440
      • = 6 2X

& BOUNDAry CONDITIONS (^) : Y =^8

  • =^1 (1440) El 8 = 10

El

= El (^2) 3 #y = -+ X Elo^ = +^4 Cl =^1448 &* E

  • E + 1440x^ +^

EN

=+ Y x y = ( ,

Elo (^) = (^) GRE

  • ECR) + 1440 (1) the R Ce =^25 , 970 y = E (^) # = +^1440 EM=^ Of = 60kv^ (8m]

+ M

= O - =

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

& =^ X =^0

: -

+ 10X^

  • (^) e5 9 ( V = v