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Page 1: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

Civil Engineering by Sandeep Jyani

Page 2: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

T - BeamBBf

Flange

Web

Df

Effective Width

Bw

Civil Engineering by Sandeep Jyani

Page 3: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

T - Beam1. Critical Neutral Axis

• 𝑥𝑐 =m𝝈𝒄𝒃𝒄

m𝝈𝒄𝒃𝒄+𝝈𝒔𝒕× 𝑑 (𝑥𝑐 = kd)

2. Actual Depth of Neutral AxisA. CASE 1: When 𝒙𝒂 lies in flange portion

𝒃𝒇 × 𝒙𝒂 ×𝒙𝒂𝟐= 𝒎𝑨𝒔𝒕 × 𝒅 − 𝒙𝒂

• 𝑀𝑅 𝑐𝑜𝑚𝑝 = 𝑏 × 𝒙𝒂 ×𝑪𝒂2

× 𝑑 −𝑥𝑎3

• 𝑀𝑅 𝑡𝑒𝑛𝑠𝑖𝑜𝑛 =𝒕𝒂𝑚×𝑚𝐴𝑠𝑡 × 𝑑 −

𝑥𝑎3

Flange

Web

𝒃𝒘

C

LA

𝒕𝒂/m

𝑪𝒂𝒙𝒂

𝒃𝒇

Civil Engineering by Sandeep Jyani

Page 4: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

T - Beam2. Actual Depth of Neutral Axis

B. CASE 2: When 𝒙𝒂 lies in web portion

𝒃𝒇 × 𝒅𝒇 × 𝒙𝒂−𝒅𝒇𝟐

+ (𝒙𝒂 − 𝒅𝒇) × 𝒃𝒘

× (𝒙𝒂 − 𝒅𝒇

𝟐) = 𝒎𝑨𝒔𝒕 × 𝒅 − 𝒙𝒂

Flange

Web

𝒃𝒘

𝒕𝒂/m

𝑪𝒂𝒙𝒂

𝒃𝒇

𝒅𝒇 C’

Civil Engineering by Sandeep Jyani

Page 5: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

T - Beam3. Moment of Resistance

Flange

Web

𝒃𝒘

𝒕𝒂/m

𝑪𝒂𝒙𝒂

𝒃𝒇

𝒅𝒇 C’𝑴𝑶𝑹𝒄𝒐𝒎𝒑 = 𝑴𝑶𝑹𝒇𝒍𝒂𝒏𝒈𝒆 +𝑴𝑶𝑹𝒘𝒆𝒃

𝑴𝑶𝑹𝒇𝒍𝒂𝒏𝒈𝒆 = 𝒃𝒇 × 𝒅𝒇 ×𝑪𝒂 + 𝑪′

𝟐× 𝒅 − 𝒚𝟏

𝑪𝒇

𝑪𝒘

ഥ𝒚𝟏

𝑪𝒇 𝑳𝑨𝒇𝒍𝒂𝒏𝒈𝒆

𝑴𝑶𝑹𝒘𝒆𝒃 = 𝒃𝒘 × (𝒙𝒂 − 𝒅𝒇) ×𝑪′

𝟐× 𝒅 − 𝒅𝒇 −

𝒙𝒂 − 𝒅𝒇

𝟑

𝑪𝒘 𝑳𝑨𝒘𝒆𝒃

𝑳𝑨𝒘𝒆𝒃

𝑳𝑨𝒇𝒍𝒂𝒏𝒈𝒆

ഥ𝒚𝟏 =𝟐𝑪′ + 𝑪𝒂

𝑪′ + 𝑪𝒂×𝒅𝒇

𝟑

Civil Engineering by Sandeep Jyani

Page 6: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

T - Beam3. Moment of Resistance

Flange

Web

𝒃𝒘

𝒕𝒂/m

𝑪𝒂𝒙𝒂

𝒃𝒇

𝒅𝒇 C’𝑴𝑶𝑹𝒕𝒆𝒏𝒔𝒊𝒐𝒏 =?

𝑴𝑶𝑹 = 𝒎𝑨𝒔𝒕 ×𝒕𝒂𝒎× 𝒅 − ഥ𝒚

𝑪𝒇

𝑪𝒘

ഥ𝒚𝟏

𝑳𝑨𝒘𝒆𝒃

𝑳𝑨𝒇𝒍𝒂𝒏𝒈𝒆

ഥ𝒚𝟐

ഥ𝒚 =𝑪𝒇 × ഥ𝒚𝟏 + 𝑪𝒘 × ഥ𝒚𝟐

𝑪𝒇 + 𝑪𝒘

ഥ𝒚𝟏 =𝟐𝑪′ + 𝑪𝒂

𝑪′ + 𝑪𝒂×𝒅𝒇

𝟑

ഥ𝒚𝟐 = 𝒅𝒇 +𝒙𝒂 − 𝒅𝒇

𝟑

Civil Engineering by Sandeep Jyani

Page 7: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

𝑇𝐻𝐸𝑅𝐸 𝐼𝑆 𝑺𝑯𝑬𝑨𝑹 𝑭𝑶𝑹𝑪𝑬

𝑊𝐻𝐸𝑅𝐸 𝑇𝐻𝐸𝑅𝐸 𝐼𝑆 𝐴 𝐶𝐻𝐴𝑁𝐺𝐸 𝐼𝑁 𝑩𝑬𝑵𝑫𝑰𝑵𝑮𝑴𝑶𝑴𝑬𝑵𝑻

𝑅𝑎𝑡𝑒 𝑜𝑓 𝑐ℎ𝑎𝑛𝑔𝑒 𝑜𝑓 𝐵𝑒𝑛𝑑𝑖𝑛𝑔 𝑚𝑜𝑚𝑒𝑛𝑡𝑖𝑠 𝑺𝑯𝑬𝑨𝑹 𝑭𝑶𝑹𝑪𝑬

Civil Engineering by Sandeep Jyani

Page 8: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

SHEAR

1. Diagonal Tension Failure• LARGE Shear Force and Less bending moment• Web shear causes cracks which progress with 45° with

horizontal2. Flexural shear Failure

• LARGE BENDING MOMENT and Less Shear Force• Such cracks are normally at 90°• Steel yields in flexural tension shear

3. Diagonal compression Failure• It occurs under LARGE Shear Force• Concrete crushes in compression due to flexural compression

• Bending in reinforced concrete beams is usually accompanied by shear, the exact analysis of which is very complex.

• However, experimental studies confirmed the following three different modes of failure due to

possible combinations of shear force and bending moment at a given section

45°

90°

Civil Engineering by Sandeep Jyani

Page 9: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

Shear

1. Shear force is resisted by the uncracked Concrete in compression region,

2. The aggregate interlocking and

3. The shear acting across longitudinal steel bars

The shear force across the steel bars is also known as Dowel Force

𝐶𝑜𝑚𝑝𝑟𝑒𝑠𝑠𝑖𝑣𝑒 𝑓𝑜𝑟𝑐𝑒 𝑖𝑛 𝑐𝑜𝑛𝑐𝑟𝑒𝑡𝑒

𝑇𝑒𝑛𝑠𝑖𝑙𝑒 𝑓𝑜𝑟𝑐𝑒𝑖𝑛 𝑠𝑡𝑒𝑒𝑙

𝐷𝑜𝑤𝑒𝑙 𝐹𝑜𝑟𝑐𝑒

Shear Force

Civil Engineering by Sandeep Jyani

Page 10: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

1. For Homogenous Section

• 𝐼 =𝐵𝐷2

12,

• ത𝑦 =𝑫

𝟐−𝒚𝟏

2+ 𝑦1

• 𝐴 =𝑫

𝟐− 𝒚𝟏 × 𝐵

𝒚𝟏ഥ𝒚

𝑫

𝟐− 𝒚𝟏

𝑩

𝑺𝒉𝒆𝒂𝒓 𝑺𝒕𝒓𝒆𝒔𝒔 =𝑽𝑨ത𝑦

𝑰𝑩

=𝑽

𝑫𝟐− 𝒚𝟏 × 𝐵

𝑫𝟐− 𝒚𝟏2

+ 𝑦1

𝑰𝑩

=𝑽

𝑫𝟐− 𝒚𝟏 × 𝐵

𝑫4+𝑦12

𝑰𝑩

=𝑽

𝑫𝟐− 𝒚𝟏 ×

𝑩2

𝑫2+ 𝑦1

𝑰𝑩

=𝑽

𝟐𝑰

𝑫𝟐

𝟐 − 𝒚𝟏𝟐

Civil Engineering by Sandeep Jyani

Page 11: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

1. For Homogenous Section

𝒚𝟏ഥ𝒚

𝑫

𝟐− 𝒚𝟏

𝑩

𝑺𝒉𝒆𝒂𝒓 𝑺𝒕𝒓𝒆𝒔𝒔 =𝑽

𝟐𝑰

𝑫

𝟐𝟐− 𝒚𝟏

𝟐

𝒚𝟏 =𝑫

𝟐, 𝑺𝒉𝒆𝒂𝒓 𝑺𝒕𝒓𝒆𝒔𝒔 = 𝟎

𝒚𝟏 = 𝟎, 𝑺𝒉𝒆𝒂𝒓 𝑺𝒕𝒓𝒆𝒔𝒔 = 𝒎𝒂𝒙𝒊𝒎𝒖𝒎

𝑭𝒐𝒓 𝒂 𝒉𝒐𝒎𝒐𝒈𝒆𝒏𝒐𝒖𝒔 𝒔𝒆𝒄𝒕𝒊𝒐𝒏,𝒔𝒉𝒂𝒑𝒆 𝒐𝒇 𝒔𝒉𝒆𝒂𝒓 𝒔𝒕𝒓𝒆𝒔𝒔 𝒅𝒊𝒂𝒈𝒓𝒂𝒎

𝒊𝒔 𝒑𝒂𝒓𝒂𝒃𝒐𝒍𝒊𝒄

Civil Engineering by Sandeep Jyani

Page 12: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

2. For Non Homogenous Section

𝒙𝒂

𝑺𝒉𝒆𝒂𝒓 𝑺𝒕𝒓𝒆𝒔𝒔 =𝑽𝑨ത𝑦

𝑰𝒆𝒒𝑩

=𝑽 𝐵 𝒙𝒂− 𝒚

𝒙𝒂− 𝒚2

+ 𝑦

𝑰𝒆𝒒𝑩

=𝑽

𝟐𝑰𝒆𝒒(𝑥𝑎 − 𝑦)(𝒙𝒂+ 𝒚)

=𝑽

𝟐𝑰𝒆𝒒(𝒙𝒂

2− 𝑦2)

𝒚

𝑺𝒉𝒆𝒂𝒓 𝑺𝒕𝒓𝒆𝒔𝒔 =𝑽

𝟐𝑰𝒆𝒒(𝒙𝒂

2− 𝑦2)

𝒚 = 𝒙𝒂, 𝑺𝒉𝒆𝒂𝒓 𝑺𝒕𝒓𝒆𝒔𝒔 = 𝟎𝒚 = 𝟎, 𝑺𝒉𝒆𝒂𝒓 𝑺𝒕𝒓𝒆𝒔𝒔 = 𝒎𝒂𝒙𝒊𝒎𝒖𝒎

𝑭𝒐𝒓 𝒂 𝑹𝑪𝑪 𝒔𝒆𝒄𝒕𝒊𝒐𝒏,𝒔𝒉𝒂𝒑𝒆 𝒐𝒇 𝒔𝒉𝒆𝒂𝒓 𝒔𝒕𝒓𝒆𝒔𝒔 𝒅𝒊𝒂𝒈𝒓𝒂𝒎

𝒊𝒔 𝒑𝒂𝒓𝒂𝒃𝒐𝒍𝒊𝒄 𝒂𝒃𝒐𝒗𝒆 𝑵𝑨 𝒂𝒏𝒅𝒓𝒆𝒄𝒕𝒂𝒏𝒈𝒖𝒍𝒂𝒓 𝒃𝒆𝒍𝒐𝒘 𝑵𝑨

Civil Engineering by Sandeep Jyani

Page 13: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

Shear Stress Below Neutral Axis

NA

MmaxM M+dM

Vmax

V V-dV

T T+dT

C C+dC

1

1 2

2

𝑨𝒕 𝒔𝒆𝒄𝒕𝒊𝒐𝒏 𝟏 − 𝟏

𝑀 = 𝐶 × 𝐿𝑒𝑣𝑒𝑟 𝑎𝑟𝑚or𝑀 = 𝑇 × 𝐿𝑒𝑣𝑒𝑟 𝑎𝑟𝑚

𝑨𝒕 𝒔𝒆𝒄𝒕𝒊𝒐𝒏 𝟐 − 𝟐

[𝑀 + 𝑑𝑀] = 𝐶 + 𝑑𝐶 × 𝐿𝑒𝑣𝑒𝑟 𝑎𝑟𝑚Or[𝑀 + 𝑑𝑀] = 𝑇 + 𝑑𝑇 × 𝐿𝑒𝑣𝑒𝑟 𝑎𝑟𝑚

… . . (1)

… . . (2)

[𝑀 + 𝑑𝑀 −𝑀] = 𝑇 + 𝑑𝑇 − 𝑇 × 𝐿𝑒𝑣𝑒𝑟 𝑎𝑟𝑚

⇒ 𝑑𝑀 = 𝑑𝑇 × 𝐿𝑒𝑣𝑒𝑟 𝑎𝑟𝑚

⇒ 𝑑𝑀 = 𝑑𝑇 × 𝑗𝑑

⇒ 𝒅𝑻 =𝒅𝑴

𝒋. 𝒅

Civil Engineering by Sandeep Jyani

Page 14: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

𝒅𝑻

𝒅𝒙

𝑩𝝉

⇒ 𝒅𝑻 =𝒅𝑴

𝒋. 𝒅

⇒ 𝒅𝑻 = 𝝉 × (𝑩 × 𝒅𝒙)𝒂𝒓𝒆𝒂 𝒐𝒇 𝒄𝒓𝒐𝒔𝒔 𝒔𝒆𝒄𝒕𝒊𝒐𝒏𝒔𝒉𝒆𝒂𝒓

𝒔𝒕𝒓𝒆𝒔𝒔

⇒𝒅𝑴

𝒋. 𝒅= 𝝉 × (𝑩 × 𝒅𝒙)

⇒ 𝝉 =𝒅𝑴

𝒅𝒙 𝑩. 𝒋. 𝒅

⇒ 𝝉 =𝑽

𝑩. 𝒋. 𝒅

Civil Engineering by Sandeep Jyani

Page 15: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

IS Code Recommendation1. As per IS code recommendation, the shear stress below the

depth of neutral axis is assumed to be constant upto effective depth d due to ineffectiveness of the concrete in the tension zone

2. As per IS code recommendation, the I (moment of inertia) is

taken as 𝐼𝑒𝑞 and that is equal to 𝑩𝒙𝒂

𝟑

𝟑+𝒎𝑨𝒔𝒕 𝒅 − 𝒙𝒂

𝟐

3. Circular section is best in carrying or resisting shear force and is assumed to be best section

4. As per IS code recommendation, the shear stress is assumed to be constant throughout the depth of the section, therefore it is considered as

𝑉

𝐵𝑑

Civil Engineering by Sandeep Jyani

Page 16: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

SHEAR

• As per IS recommendations, the beam can be designed either for maximum shear force or for maximum shear force at critical section.

• As per IS code 456, critical section is at a distance of ‘d’ from the face of the support.

• Concrete beams are expected to crack in flexure, with such cracks forming perpendicular to longitudinal tension reinforcement, i.e., perpendicular also to a free edge.

VmaxV

Civil Engineering by Sandeep Jyani

Page 17: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

1. NOMINAL SHEAR STRESS• It is the average shear stress developed in a cross section.

• It is generally denoted by

𝝉𝒗 =𝑽

𝑩𝒅

𝑽 = 𝝉𝒗 𝑩 𝒅2. Design Shear Strength of Reinforced Concrete • 𝝉𝒄 is the shear strength of reinforced concrete.

• It depends upon grade of concrete and % of main tension reinforcement.

• The shear force resisted by the concrete

𝑽𝒄 = 𝝉𝒄 𝑩 𝒅

Civil Engineering by Sandeep Jyani

Page 18: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

Design Shear Strength of Reinforced Concrete

Civil Engineering by Sandeep Jyani

Page 19: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

3. Stress in Shear Reinforcement

𝑵𝒐𝒎𝒊𝒏𝒂𝒍 𝒔𝒉𝒆𝒂𝒓 𝒇𝒐𝒓𝒄𝒆 𝑽 = 𝝉𝒗 𝑩 𝒅𝑺𝒉𝒆𝒂𝒓 𝒇𝒐𝒓𝒄𝒆 𝒓𝒆𝒔𝒊𝒔𝒕𝒆𝒅 𝒃𝒚 𝒄𝒐𝒏𝒄𝒓𝒆𝒕𝒆 𝑽𝒄 = 𝝉𝒄 𝑩 𝒅

The remaining shear force is to be resisted by the Shear reinforcement (stirrups):𝑽𝒔 = 𝑽− 𝑽𝒄

𝑽𝒔 = (𝝉𝒗− 𝝉𝒄)𝑩 𝒅

4. Maximum Shear Stress 𝝉𝒄 𝒎𝒂𝒙• The shear stress developed in the beam should not be more than

maximum shear stress of the beam

• 𝝉𝒄𝒎𝒂𝒙 depends only on the grade of concrete

• If 𝝉𝒗 is greater than 𝝉𝒄𝒎𝒂𝒙 then the size of beam has to be revised

Civil Engineering by Sandeep Jyani

Page 20: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

4. Maximum Shear Stress 𝝉𝒄 𝒎𝒂𝒙

• The shear stress developed in the beam should not be more than maximum shear stress of the beam

• 𝝉𝒄𝒎𝒂𝒙 depends only on the grade of concrete

• If 𝝉𝒗 is greater than 𝝉𝒄𝒎𝒂𝒙 then the size of beam has to be revised

• 𝝉𝒄𝒎𝒂𝒙 > 𝝉𝒗 VALID

• 𝝉𝒄𝒎𝒂𝒙 < 𝝉𝒗 INVALID (SECTION TO BE REVISED, NO OTHER OPTION)

Civil Engineering by Sandeep Jyani

Page 21: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

Maximum shear stress, 𝝉𝒄 𝒎𝒂𝒙 in N/mm2

Civil Engineering by Sandeep Jyani

Page 22: Civil Engineering by Sandeep Jyani · C LA /m Civil Engineering by Sandeep Jyani. T - Beam 2. Actual Depth of Neutral Axis B. CASE 2: When

Minimum Shear Reinforcement• (Clause. 40.3, 26.5.1.5 and 26.5.1.6 of IS 456)

• Minimum shear reinforcement has to be provided even when 𝝉𝒗 is less than 𝝉𝒄

• 𝝉𝒗 < 𝝉𝒄 minimum shear reinforcement required

• 𝝉𝒗 <0.5 𝝉𝒄 No shear reinforcement is required

• The minimum shear reinforcement in the form of stirrups shall be provided such that

• Asv = total cross-sectional area of stirrup legs effective in shear• sv = stirrup spacing along the length of the member• b = breadth of the beam or breadth of the web of the web of flanged beam bw, and• fy = characteristic strength of the stirrup reinforcement in N/mm2 which shall not be

taken greater than 415 N/mm2 .

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Minimum Shear Reinforcement

• 𝝉𝒗 < 𝝉𝒄 minimum shear reinforcement required

• 𝝉𝒗 <0.5 𝝉𝒄 No shear reinforcement is required

• 𝝉𝒗 > 𝝉𝒄 Design shear reinforcement (vertical of inclined)

• 𝝉𝒗 > 𝝉𝒄𝒎𝒂𝒙 Redesign the section

Civil Engineering by Sandeep Jyani

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Minimum Shear Reinforcement

• Clause 26.5.1.5 of IS 456 stipulates that the maximum spacing of shear reinforcement measured along the axis of the member shall not be more than 0.75 d for vertical stirrups and d for inclined stirrups at 45° , where d is the effective depth of the section.

1. Sv < 0.75 d Vertical shear Reinforcement

2. Sv < d Inclined shear Reinforcement

3. However, the spacing shall not exceed 300 mm in any case.

Civil Engineering by Sandeep Jyani

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Que: If depth of beam is 300mm, find spacing for shear reinforcement

Solution:

Civil Engineering by Sandeep Jyani

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Que: If depth of beam is 300mm, find spacing for shear reinforcement

Solution:

i. For vertical stirrup• 0.75d = 0.75 x 300 =225mm

ii. For inclined stirrup• d=300mm

iii. For any case maximum r/f =300 mm

Answer: minimum of all these = (i)=225mm

Civil Engineering by Sandeep Jyani

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The minimum shear reinforcement is provided for the following:

1. Any sudden failure of beams is prevented if concrete cover bursts and the bond to the tension steel is lost.

2. Brittle shear failure is arrested which would have occurred without shear reinforcement.

3. Tension failure is prevented which would have occurred due to shrinkage, thermal stresses and internal cracking in beams.

4. To hold the reinforcement in place when concrete is poured

5. Section becomes effective with the tie effect of the compression steel

Civil Engineering by Sandeep Jyani

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Objective question

𝝉𝒄 𝒎𝒂𝒙

𝝉𝒄

𝒈𝒓𝒂𝒅𝒆 𝒐𝒇 𝒄𝒐𝒏𝒄𝒓𝒆𝒕𝒆

𝒈𝒓𝒂𝒅𝒆 𝒐𝒇 𝒄𝒐𝒏𝒄𝒓𝒆𝒕𝒆

𝒑𝒆𝒓𝒄𝒆𝒏𝒕𝒂𝒈𝒆 𝒐𝒇 𝒕𝒆𝒏𝒔𝒊𝒍𝒆 𝒓𝒆𝒊𝒏𝒇𝒐𝒓𝒄𝒆𝒎𝒆𝒏𝒕

Civil Engineering by Sandeep Jyani

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Civil Engineering by Sandeep Jyani

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