In a boundary value problem, what's the difference between "essential boundary conditions" and "natural boundary conditions"?
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In the context of a variational problem for a functional
$$I[q]~:=~\int_{t_i}^{t_f} \! dt ~L(q,\dot{q},t),\qquad \dot{q}~\equiv~ \frac{dq}{dt},$$
defined on an interval $[t_i,t_f]\subseteq \mathbb{R}$, the types of boundary conditions (BC) are defined as follows:
Essential/Dirichlet BC: $\quad q(t_i)~=~q_i\quad\text{and}\quad q(t_f)~=~q_f.$
Natural BC: $\quad p(t_i)~=~0\quad\text{and}\quad p(t_f)~=~0.$
Here $$p~:=~\frac{\partial L}{\partial \dot{q}} $$ is the canonical/conjugate momentum.
See also e.g. in my related Phys.SE answer here. The types of BC generalize to higher-dimensional regions.
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What will be the natural Boundary Conditions if instead of $L(q,\dot{q},t)$ we have $L(q,\dot{q},\ddot{q},t)$? – TheStudent Jul 29 '21 at 10:27
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Hi @honey kumar. You might be interested in my Phys.SE answer here. – Qmechanic Jul 31 '21 at 10:48
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Thankyou @Qmechanic – TheStudent Jul 31 '21 at 14:25