Can anyone explain the derivation of the formula for cantilever oscillations?

[ash1098]

[SOLVED] Cantilever Investigation

1.Hi,

I am writing a report on cantilever oscillations, my experiment involves fixing different cantilvers e.g. a ruler to the end of a table then measuring the period and height of oscillations while varing the mass attached to the cantilever, and other varients e.g. length of cantilever.

2. I have found these two formulae: (Shown much more clearly in attachments)

T= 2(pi)*[(4ML^3)/(bd^3E)]^1/2

and:

h= 4MgL^3/Ebd^3

where:
b= width of cantilever
d= thickness of cantilever
E= Youngs Modulus
M=Mass
L=Lenght of cantilever
T=period of oscillations
h=height of oscillation


3. I have looked at eqn's involving Hooke's and simple harmonic motion but cannot work out how these formulae have been derived.

Does anyone know how these formulae where derived, or where I can find information on this in general?

Thanks.

ash.

p.s. I have written out the formulae using math open office and attached them in pdf if it helps make them easier to read.

 

[rock.freak667]

Well I have done a lab to find the Young's Modulus of a loaded cantilever and this is theory which is written down on the paper:

The depression,s,due to a load W(=Mg) at the end of a cantilever of length,l, is

s=\frac{Wl^3}{3IE}

This strain brings into play internal stresses which produce a restoring force equal to W, i.e. equal to \frac{3IEs}{l^3}.

If the acceleration of the load \frac{d^2s}{dt^2} when the cantilever is displaced to produce vertical oscillations,then

M\frac{d^2s}{dt^2}=\frac{-3IE}{l^3}s

OR
\frac{d^2s}{dt^2}+\frac{3IE}{Ml^3}s=0

Hence the motion is Simple harmonic and the periodic time,T, is

T=2\pi \sqrt{\frac{Ml^3}{3IE}}

from which

E=\frac{4\pi^2Ml^3}{3IT^2}

For a beam of rectangular section:
I=\frac{bd^3}{12}
I hope that helps in some way

 

[ash1098]

Thanks for your reply rock.freak it's really really useful, just one question:

why does T=2\pi \sqrt{\frac{Ml^3}{3IE}}

Thanks, ash.

 

[rock.freak667]

Well from
M\frac{d^2s}{dt^2}=\frac{-3IE}{l^3}s

\frac{d^2s}{dt^2}=\frac{-3IE}{Ml^3}s

and that is of the form a=-\omega^2 s where a=\frac{d^2s}{dt^2}

so from that

\omega=\sqrt{\frac{3IE}{Ml^3}}

and since it moves with SHM, the period,T, is given by

T=\frac{2\pi}{\omega}

 

[ash1098]

Oh yeah I see it now, Thanks a lot.

Ash.