D'Alembert's Principle
By Philip Ellison on Thursday, February
21, 2002 - 09:57 pm:
In his answer to one of the STEP questions I posted on this
board, Arun refers to "D'Alembert's Principle" and told me that
it involves using "inertial forces" on bodies in static
equilibrium. Could somebody please explain this principle or
direct me to a website with information on it (as I cannot find
it on the "World of Mathematics" site). If possible, please reply
tonight.
Thanks for any help
By Kerwin Hui on Friday, February 22, 2002
- 01:17 am:
D'Alembert's principle is usually known
as the principle of virtual work. It states that if a system is
in equilibrium, then the work done (by external forces) in a
virtual (infinitesimal) displacement is zero.
Kerwin
By Philip Ellison on Friday, February 22,
2002 - 06:27 pm:
Could you please elaborate on this definition (or give
examples of how to use it, etc.)? The principle seems
self-evident, but how to apply it less so.
Thanks
By Arun Iyer on Saturday, February 23,
2002 - 12:14 pm:
Phillip,
I will try and explain D'Alembert's principle to the best of my
abilities...
Consider a particle P of mass m having acceleration a when acted upon by
several forces(say F1 and F2).Let
be the resultant of these
forces...
Now,by Newton's second law,
where the acceleration of the particle is in the direction of the resultant
force
.
This equation is referred to as the ''equation of motion of particle P''
This equation can be written in the form...
which means that the resultant of the external forces (
) and the force
(-m a) is zero. The force (-m a) is called the inertia force. (The
inertia of the body can be defined as resistance to the change in the
condition of rest or of uniform motion of the body.)
Now the equation is written as...
where inertia force = -m a
this equation is called as the equation of dynamic equilibrium of the particle P.
Now the concept of D'Alemberts principle is that..."to write
the equation of dynamic equilibrium of a particle, add a
fictitious force equal to the inertia force to the external force
acting on the particle and equate the sum to zero."
Hope this helps...
love arun
By Arun Iyer on Saturday, February 23,
2002 - 12:16 pm:
kerwin,
i don't know how D'Alembert's principle is related to the
principle of virtual work...i think you may have go it
wrong!!(Please do correct me if i am wrong!!!)
love arun
By Kerwin Hui on Saturday, February 23,
2002 - 02:08 pm:
Arun,
There are two versions of D'Alembert's principle (and different books have
different nomenclature, as always). One version, which is also called the
principle of virtual work, states that the condition for equilibrium of a
system is that the virtual work of the applied forces is zero. The other
version, which is also known as the dynamic principle of virtual work, is
roughly what you had stated. More precisely, this version states that
| dW= |
å
i
|
(Fi- dPi/dt)·dri=0
|
where Fi, Pi and dri are the external force
on the ith particle, the momentum of the ith particle, and the virtual
displacement of the ith particle respectively. This can be deduced from
Newton's second law Fi +fi = dPi /dt and
assuming the internal forces fi do no work (which is often the
case). If the particle is in equilibrium, then Pi is constant for
every i, so we recover the principle of virtual work.
Kerwin
By Arun Iyer on Saturday, February 23,
2002 - 05:32 pm:
Hmmm!!!i see!!
i know the principle of virtual work but never knew that its also
called the D'Alembert's principle!!(thanks for the info
Kerwin!!)
love arun
P.S-> i really like principle of virtual work ,it makes so
many problems of mechanics simple...!!