1 / 8

Plain & Reinforced Concrete-1 CE3601

Plain & Reinforced Concrete-1 CE3601. Lecture # 6 21 rd Feb 2012 Flexural Analysis and Design of Beams. Plain & Reinforced Concrete-1. Cracked Transformed Section When tensile stress cross f r , crack appear on the tension face of beam. Tensile strength of concrete is neglected.

dorit
Download Presentation

Plain & Reinforced Concrete-1 CE3601

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Plain & Reinforced Concrete-1CE3601 Lecture # 621rd Feb 2012 Flexural Analysis and Design of Beams

  2. Plain & Reinforced Concrete-1 Cracked Transformed Section When tensile stress cross fr, crack appear on the tension face of beam. • Tensile strength of concrete is neglected. • All the concrete on the tension side of N.A. is neglected. Only the Shaded area of cross-section is considered effective. Concrete N.A Steel

  3. Plain & Reinforced Concrete-1 Cracked Transformed Section (contd…) b εc fc Cc kd N.A. h d nAs la = jd fs T = Asfs εs Cracked Transformed Section Internal Force Diagram Stress Diagram Strain Diagram When the tension side is cracked the concrete becomes ineffective but the strains goes on increasing. The steel comes in to action to take the tension.

  4. Plain & Reinforced Concrete-1 b Cracked Transformed Section (contd…) Calculations for“k”, taking top face as reference kd = [b x kd x kd/2 + nAsd]/ [b x kd + nAs] b x (kd)2 + nAs kd = b x (kd)2/2 + nAsd b x (kd)2/2 = nAsd - nAs kd b x (kd)2/2 = (1-k) nAsd bd2/2 k2 = (1-k) nρbd2 k2 = 2(1-k) nρ k2 + 2nρ k - 2nρ = 0 kd d nAs Cracked Transformed Section ρ = As / bd

  5. Plain & Reinforced Concrete-1 b Cracked Transformed Section (contd…) k2 + 2nρ k - 2nρ = 0 k = [ -2nρ ± √ (4n2ρ2 + 8nρ) ] /2 k = [ -nρ ± √ (n2ρ2 + 2nρ) ] k = √ (n2ρ2 + 2nρ) -nρ Taking only positive value as distance can’t be negative kd d nAs Cracked Transformed Section

  6. Plain & Reinforced Concrete-1 fc Cracked Transformed Section (contd…) Value of “j” jd = d – kd/3 J = 1 – k/3 Cc = volume of stress diagram Cc = ½ kd x fc x b Cc = fc/2 x kdb T = Asfs = nfcAs b Cc kd d N.A jd T = Asfs

  7. Plain & Reinforced Concrete-1 Cracked Transformed Section (contd…) Resisting Moment Capacity For longitudinal equilibrium T = Cc Mr = T x jd = Cc x jd Mr = Asfs x jd = fc/2 x kdb x jd ------------- 1 FOR MAXIMUM VALUE RESISTING MOMENT Put in eq-1 fs = 0.5 fy for grade 300 steel fs = 0.4 fy for grade 420 steel fs = Maximum allowable tensile stress in steel fc= 0.45 fc’ fc = Maximum allowable concrete stress

  8. Concluded

More Related