Applied Physics I: Chapter 1: Properties of Matter - Elasticity

Experimental Determination of Youngs modulus - Non uniform Bending

Experimental Determination of Youngs modulus - Non uniform Bending

It consists of a beam, symmetrically supported on the two knife edges A and B. A weight hanger is suspended at the centre (C) of the beam my means or a loop (or) thread.

EXPERIMENTAL DETERMINATION OF YOUNGS MODULUS - NON UNIFORM BENDING

 

STATICAL METHOD

 

Description:

It consists of a beam, symmetrically supported on the two knife edges A and B. A weight hanger is suspended at the centre (C) of the beam my means or a loop (or) thread. A pin is fixed vertically at 'C' by some wax as shown in Fig 1.14. In order to focus the tip of the pin a travelling microscope (M) is placed in front of this arrangement.


 

Procedure:

Taking the weight hanger as the dead load (W) the microscope is adjusted and the tip of the pin is made to coincide with the horizontal cross wire. The reading is noted from the vertical scale of the microscope.

The weights are added (loaded) in steps of m, 2m, 3m kilograms and the corresponding readings are noted from the vertical scale of the microscope. The same procedure is repeated while unloading and the readings are tabulated in the tabular column as shown. The mean depression 'y' is found for a load of M kg.


Theoretically, we know the depression produced is

 .....(1)

Where ‘l’ be the length of the beam (i.e.) the distance between the knife edge. If 'b' is the breadth of the beam and 'd' is the thickness of the beam, then

The geometical of moment of inertia Ig = bd3 / 12                  ...(2)

Also the weight W = Mg      ...(3)

Substituting eqn.(2) and eqn.(3) in eqn.(1), we get


Rearranging eqn. (4) we get

Youngs modulus


.....(5)

Substituting the mean value of (M/y), from the tabular column, the youngs modulus Y can be determined.

 

Graphical Method (or) Dynamical Method:

A graph is drawn taking load. 'M' along x axis and depression (y) along y axis. It will be a straight line as shown in Fig.1.15. The slope of the graph gives the value of y/M. Eqn.(5) can be written as Y = gl3/4bd3 . 1/slope



Substituting the slope value in the given formula the youngs modulus can be calculated.

 

Applied Physics I: Chapter 1: Properties of Matter - Elasticity : Tag: Applied Physics : - Experimental Determination of Youngs modulus - Non uniform Bending


Applied Physics I: Chapter 1: Properties of Matter - Elasticity



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