Continuous Rc Beams
-
Upload
pranav-gairola -
Category
Documents
-
view
67 -
download
1
Transcript of Continuous Rc Beams
![Page 1: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/1.jpg)
OUTLINE
CONTINUOUS R. C. BEAMS
• Idealizations in structural analysis1. Span2. Rigidity of Supports 3. Moment of Inertia (MI) of spans4. Loading 5. Elastic methods of analysis
![Page 2: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/2.jpg)
1. SPAN
CONTINUOUS R. C. BEAMS
Idealization in span calculation• Width of simple supports is taken as zero
Concept of Effective span • For simply supported beam or slab• For continuous beam or slab• For cantilever• For frame members
![Page 3: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/3.jpg)
1. SPAN
CONTINUOUS R. C. BEAMS
Effective span for simply supported beams or members not built integrally with supports• Clear span + Effective depth le = ln + d
OR• Centre-to-centre of supports le = l
Whichever is LESS
![Page 4: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/4.jpg)
1. SPAN
CONTINUOUS R. C. BEAMS
Effective span for continuous beams or slabs with support width < clear span/ 12• Clear span + Effective depth le = ln + d
OR• Centre-to-centre of supports le = l
Whichever is LESS
![Page 5: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/5.jpg)
1. SPAN
CONTINUOUS R. C. BEAMS
Effective span for continuous beams or slabs with support width > clear span/ 12 OR > 600 mm
For end span with fixed endeffective span = clear span le = ln
For end span with free endle = ln + d/2 = ln + support width/2
![Page 6: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/6.jpg)
1. SPAN
CONTINUOUS R. C. BEAMS
For end span with free endle = ln + d/2 = ln + support width/2
![Page 7: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/7.jpg)
1. SPAN
CONTINUOUS R. C. BEAMS
Effective span for cantilever span is For a cantilever span, the effective length is length to face of support + d/2
For cantilever span of continuous beam, length to centre of support
le = ln + d/2 le = l
ln l
![Page 8: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/8.jpg)
1. SPAN
CONTINUOUS R. C. BEAMS
![Page 9: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/9.jpg)
2. Supports
CONTINUOUS R. C. BEAMS
Idealization in span calculation• Supports are unyielding
Support sinking or rotation -> secondary forces • Redistribution of BMs occurs• BM can become positive over continuous
supports, and positive BM at centre increases• Beam fails at support and then at centre
Redistribution of BMs caused by support movement has to accounted in structural Analysis
![Page 10: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/10.jpg)
3. STIFFNES
S
CONTINUOUS R. C. BEAMS
Idealization in stiffness• MI remains constant throughout the span
Moment of Inertial (MI) at a section depends on• Amount and location of reinforcement • Extent of cracking• Shape of concrete in compression
Relative stiffness (I/L)should be calculated consistently• Gross section MI (Or)• Transformed section MI (Or)• Cracked section MI
![Page 11: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/11.jpg)
4. LOADIN
G
CONTINUOUS R. C. BEAMS
Idealization in loading• The loads on all spans are known (fixed) values
But,• The load values are only characteristic values• Live load may or may not be present on a span• Change in loading on any portion can affect
BMs and SF s on a given span
![Page 12: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/12.jpg)
4. LOADIN
G
CONTINUOUS R. C. BEAMS
So,• BMD is also characteristic (i.e., it has
variability)• Live load patterns that give worst effect should
be considered• Appropriate substitute frames are to be
selected for the stress-resultant .
![Page 13: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/13.jpg)
4. LOADIN
G
CONTINUOUS R. C. BEAMS
Live Load Patterns• For max. + ve moment in span S, load the span
under consideration and also the alternate spans
S
![Page 14: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/14.jpg)
4. LOADIN
G
CONTINUOUS R. C. BEAMS
P
Live Load Patterns• For max. + ve moment at support P, unload
spans on either side of the support P and load the alternate spans on either side
![Page 15: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/15.jpg)
4. LOADIN
G
CONTINUOUS R. C. BEAMS
P
Live Load Patterns• For max. - ve moment at support P and max.
SF, Load adjacent spans on both sides of the support P and also the spans alternate to these
![Page 16: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/16.jpg)
4. LOADIN
G
CONTINUOUS R. C. BEAMS
S
Live Load Patterns• For max. - ve moment in span S, load the spans
adjoining the span S
![Page 17: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/17.jpg)
OUTLINE
CONTINUOUS R. C. BEAMS
• Moment redistribution in indeterminate beams• Stages leading to collapse• Equilibrium equations govern all stages• Load Vs moments• Design problem •Where moment redistribution can be done?• How much moment can be redistributed• Numerical problems
![Page 18: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/18.jpg)
OUTLINE
CONTINUOUS R. C. BEAMS
• Advantages of moment redistribution•Assumptions• in elastic analysis• in moment redistribution• Limitations on moment redistribution• IS456 about moment redistribution• Use of IS code coefficients (simplified method for moment redistribution analysis)• Design for redistributed BMD
![Page 19: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/19.jpg)
CONTINUOUS R. C. BEAMS
Distribution (shape) of BMD
6PL/32
5PL/32
L L
P P
Elastic Bending Moment Diagram
-+ +
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 20: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/20.jpg)
CONTINUOUS R. C. BEAMS
Redistribution (reshaping) of BMD
6PL/32 = Mp-
5PL/32
L L
P P
At first Plastic Hinge formation
-+ +
Plastic hinge
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 21: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/21.jpg)
CONTINUOUS R. C. BEAMS
Redistribution (reshaping) of BMD
6PL/32 = Mp-
Mp+
L L
Pu
At collapse (Second Plastic Hinge formation)
-+ +
Pu
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 22: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/22.jpg)
CONTINUOUS R. C. BEAMS
Equilibrium conditions
L L
P
At collapse (Second Plastic Hinge formation)
P
M+
M-
R1 = 2M+/L
2P- 2R1
P- R1
P- R1
M+
2M+ + M- = PL/2
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 23: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/23.jpg)
CONTINUOUS R. C. BEAMS
Relation between moments and load2M+ + M- = PL/2
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 24: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/24.jpg)
CONTINUOUS R. C. BEAMS
Need for BM Envelope
MO
MEN
T RE
DIS
TRIB
UTI
ON
Elastic BMDFactored BMDRedistributed BMD
![Page 25: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/25.jpg)
CONTINUOUS R. C. BEAMS
Distribution of BMs (BMD)
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 26: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/26.jpg)
CONTINUOUS R. C. BEAMS
Redistributed BMD
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 27: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/27.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Steps in structural analysis for redistribution of moments
1. Perform Elastic Structural Analysis to get elastic BMD2. Mark the points of contra-flexure3. Reduce the maximum moment by x% 4. Perform equilibrium analysis for getting redistributed BMD5. Obtain the points of contra-flexure 6. Draw envelopes of (x times elastic BMD + redistributed BMD)
![Page 28: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/28.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example
Q. Draw the design bending moment diagram of the beam of a RC fixed beam clamped at both ends and carrying ultimate uniformly distributed load of 24 kN/m with full redistribution of 30 per cent as per IS 456.
![Page 29: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/29.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example
![Page 30: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/30.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example
![Page 31: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/31.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example
![Page 32: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/32.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example - Question
Q. Draw envelope of the design moments of the two-span continuous beam shown in Fig. 15.38.7a, carrying characteristic live load of 35 kN/m in addition to its characteristic self-weight. The cross-section of the beam is 300 mm × 700 mm.
![Page 33: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/33.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example – Load cases to be considered
Three load cases: 1. DL on both spans + LL on both spans2. DL on both spans + LL on span AB only3. DL on both spans + LL on span BC only
Load Case 1
Load Case 2
Load Case 3 is a mirror image of Load case 2 . SO need not be considered separately
![Page 34: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/34.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example – Case 1 – Elastic and redistributed BMDs
![Page 35: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/35.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example – Load Case 1 – Points of contra-flexure
![Page 36: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/36.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example – Load Case 2 – loading and elastic BMDs
![Page 37: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/37.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example – Load Case 2 – Elastic BMD using MD
Member AB BA BC CB D.F 1.0 0.5 0.5 1.0 F.E.M + 322.0 - 322.0 + 28.0 - 28.0 Balanced Moment - 322.0 + 147.0 + 147.0 + 28.0 Carry over Moment - 161.0 + 14.0 - Balanced Moment - + 73.5 + 73.5 - Total Moment 0.0 - 262.5 + 262.5 0.0
![Page 38: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/38.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example – Load Case 2 – redistributed BMDs
![Page 39: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/39.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
Illustrative Example – Load Case 1 & 2 – BMD Envelop
The envelop is drawn from x times elastic BMD s of case
1,2 and 3 +
redistributed BMD of case 1,2 and 3)
![Page 40: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/40.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
1. Gives realistic picture of the load carrying capacity of indeterminate structures
2. Results in economical designs3. Designer gets some freedom to choose the design moments. This
helps to avoid congested reinforcement designs
Advantages of moment redistribution
![Page 41: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/41.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
1. Ultimate moments of resistance of the section are Mu
+ and Mu-
2. No premature shear failure occurs before the collapse load
3. Moment curvature relation is idealized bilinear curve
4. All sections have the same constant value of EI up to collapse
5. Self-weight of the beam is negligible
Assumptions used in the concept of moment redistribution
1. Sufficient plastic rotations at critical sections2. The extent of cracking should not affect the serviceability requirements
Conditions to be fulfilled to apply moment redistribution
![Page 42: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/42.jpg)
MOMEN
T REDISTRIBUTION
CONTINUOUS R. C. BEAMS
1. Moment of inertia (MI) does not vary within a span2. Supports do not yield3. Supports are knife-edged (i.e support width = zero)
Assumptions used in Elastic analysis of beams
1. In calculating the ratios of MI of adjacent spans, follow the same principle (i.e use either gross section or transformed section for all spans)
2. Support settlements are to be accounted in calculating elastic BMD 3. The concept of effective length is to be used (Cl. 22.2 of IS456-2000)
Conditions to be fulfilled to use elastic analysis
![Page 43: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/43.jpg)
CONTINUOUS R. C. BEAMS
IS Code stipulation
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 44: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/44.jpg)
CONTINUOUS R. C. BEAMS
IS Code stipulation
MO
MEN
T RE
DIS
TRIB
UTI
ON
![Page 45: Continuous Rc Beams](https://reader033.fdocuments.us/reader033/viewer/2022061109/5450f2f6b1af9f0d098b4fab/html5/thumbnails/45.jpg)
CONTINUOUS R. C. BEAMS
Simplified method based on IS Code coefficients
MO
MEN
T RE
DIS
TRIB
UTI
ON