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Course No: CE 416 Course Title :Pre-stressed Concrete Lab SOLVING STATICALLY INDETERMINATE STRUCTURE BY MOMENT AREA THEOREM Submitted by Name-Nabiha Nusrat ID no# 10.01.03.022 Submitted to Munsi Galib Muktadir Lecturer, & Sabreena Nasrin Lecturer, Ahsanullah University of Science And Technology

Moment area theorem presentation

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this my first presentation...i try my best to make easy for the viewers.

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Page 1: Moment area theorem presentation

Course No: CE 416 Course Title :Pre-stressed Concrete Lab

SOLVING STATICALLY

INDETERMINATE STRUCTURE BY

MOMENT AREA THEOREM

Submitted by

Name-Nabiha Nusrat

ID no# 10.01.03.022

Submitted to

Munsi Galib Muktadir

Lecturer,

&

Sabreena Nasrin

Lecturer,

Ahsanullah University of Science And Technology

Page 2: Moment area theorem presentation

INTRODUCTION

There are many methods for solving indeterminate structures such as

moment distribution method, slope deflection method, stiffness method etc.

Moment area method is another one.

The idea of moment area theorem was developed by Otto Mohr and later

started formally by Charles E. Greene in 1873.It is just an alternative method

for solving deflection problems.

In this method we will establish a procedure that utilizes the area of the

moment diagrams [actually, the M/EI diagrams] to evaluate the slope or

deflection at selected points along the axis of a beam or frame.

Page 3: Moment area theorem presentation

Scope of the study

In numerous engineering applications where deflection of beams must be

determine, the loading is complex and cross sectional areas of the beam vary.

When the superposition technique of indeterminate beam accelerated

according to following reasons restrained and continues beams differ from the

simply supported beams mainly by the presence of redundant moment at the

supports then moment area method can be used.

Page 4: Moment area theorem presentation

theorem

Theorem 1 :The change in slope between any two points on the elastic

curve equals the area of the M/EI diagram between two points.

Figure : Interpretation of small change in an element

Page 5: Moment area theorem presentation

Theorem(Continue)Theorem 2: The vertical deviation of the tangent at a point A on the elastic

curve with respect to the tangent extended from another B equals the moment

of the area under the M/EI diagram between the two points A and B. this

moment computed about point A where the deviation is to be determine.

Figure : Vertical deviation

Page 6: Moment area theorem presentation

Theorem(Continue)This method requires an accurate sketch of the deflected shape, employs above

two theorems. Theorem 1 is used to calculate a change in slope between two

points on the elastic curve And Theorem 2 is used to compute the vertical

distance (called a tangential deviation) between a point on the elastic curve and

a line tangent to the elastic curve at a second point.

Figure : Moment area theorem.

Page 7: Moment area theorem presentation

process Process to Draw M/EI diagram 

1. Determine a redundant reaction, that establish the numerical values for the

bending moment diagram.

2. Divided moment diagram by EI. Plot the value and sketch the M/EI

Process to Draw Elastic Curve 

1 Draw an exaggerated view of the beam’s curve. Recall that points of zero slope

occur at fixed supports and zero displacement occurs at all fixed, pin and roller

supports

2. If it becomes difficult to draw the general shape of the elastic curve, use the

M/EI diagram. Realize that when the beam is subjected to a positive moment the

beam bends concave up, where negative he negative moments bends the beam

concave down. And change in curvature occurs where the moment of the beam is

zero.

Page 8: Moment area theorem presentation

process(Continue) Process to Calculate Deviation 1. Apply theorem 1 to determine the angle between two tangents and theorem 2

to determine vertical deviation between these tangents.

2. Realize that theorem 2 in general will not yield the displacement of a point on the elastic curve. When applied properly it will only give the vertical distance or deviation of a tangent at a point A on the elastic curve from the tangent at B.

3. After applying either theorem 1 or theorem 2 the algebraic sign of the answer can be verified from the angle or deviation as indicated on the elastic curve.

Page 9: Moment area theorem presentation

problemFind the maximum downward deflection of the small aluminum beam

shown in figure due to an applied force P=100N. The beam constant

flexure rigidity EI=60N.

Page 10: Moment area theorem presentation

Problem(Continue)

Solution: The solution of this problem consists of two parts. First a

redundant reaction must be determined to establish the numerical values

for the bending moment diagram. Then the usual moment-area procedure

is applied to find the deflection.

Page 11: Moment area theorem presentation

Problem(Continue)

By assuming the beam is released from the redundant end moment, a simple

beam-moment diagram is constructed as given here.

The moment diagram of known shape due to the unknown redundant

moment

is shown on the diagram below again.

Page 12: Moment area theorem presentation

Problem(Continue)

,

Page 13: Moment area theorem presentation

Problem(Continue)

Page 14: Moment area theorem presentation

Problem(Continue)

The maximum deflection occurs where the tangent to the elastic curve is

horizontal, point C in the figure. Hence by noting that the tangent at A is also

horizontal and using the first moment theorem point C is located. When

hatched area in the figure having opposite signs are equal, that is, at a

distance 2a = 2(4.2/56.8) = 0.148 m from A. The deviation gives the

deflection of point C.

Page 15: Moment area theorem presentation

thank you