Kinematic equations are constrained equations found in dynamics of body.
In the mechanics, the constraint that is incurred on is to have constant
acceleration on a body with mass m.
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Determinant is used in eigenvalue equations and other important.
The simplest case is 2 x 2 determinant,
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In the case of 3 x 3 determinant,
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Larger determinants can be solved by similar techique used in going from
2 x 2 to 3 x 3 determinant.
Setting up equations of motion in terms of force can be rather nuisance.
It is particularly true when there are many two-body interactions.
The general procedure is to set up Lagrangian equations of motion to
make them into matrix form.
The Lagrangian function is defined by
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where
T is kinetic energy and
V is potential energy.
The variables are in terms of
ith coordinate
qi, and
is the velocity associated with
qi
(
q with a dot and a double-dot on top
indicates first derivative in time and second derivative, respecitively),
and
t is time.
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The above equation for potential energy is for harmonic motion of masses
in linear Hooke's law forces between them.
Then, the dynamical equation, called Lagrange's equation, is obtained
by the following.
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Let us now use an example. Let us write dynamical equation for
molecular vibration in one dimension. Easiest one perhaps is the
CO
2, as shown below.
Figure A1. CO2 molecule and its coordinates
The Lagrangian is written as
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We now need to subject Eqn. A11 to Eqn. A10 for each of ith
component. The first term on the left-hand side of A10 is
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where
mi is the mass associated with
xi
coordinate. You can easily see it that by taking the derivative of the
first three terms of the right-hand side of Eqn. A11, and subsequently
taking the time-derivative.
The second term on the left-hand side of A10 is
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We can rewrite Eqns. A12 and A13 into three simultaneous linear equations
containing given
i component,
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This gives the equations of motion to be solved.