Does $\frac{\partial^2 L}{\partial q\partial \dot q}=0$?

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The discussion centers on the expression $$\frac{\partial^2 L}{\partial q\partial \dot q}$$ in the context of Lagrangian mechanics. It is established that this expression does not equal zero, as demonstrated by examples where $$L = q^2 \dot{q}$$ yields $$\frac{\partial^2 L}{\partial q\partial \dot q} = 2q$$. The participants clarify that $$q$$ and $$\dot{q}$$ are independent variables in the Lagrangian framework, not functions of time unless evaluated on a solution to the equations of motion. The conversation emphasizes the importance of understanding the role of additional terms in the Lagrangian and their impact on derivatives.

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Leo Liu
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Homework Statement
.
Relevant Equations
.
This is a conceptual question.
Suppose the lagrangian of a system in generalized coordinates is $$L(q,\dot q,t)$$
If the following expression arises in calculations$$\frac{\partial^2 L}{\partial q\partial \dot q}\,,$$
does it equal to 0?
My reasoning is that since ##\dot q## and ##q## are functions of time, the expression above equals 0. Am I right?
Thanks :)
 
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Say Force
\frac{\partial L}{\partial q}=-k \cdot{\dot{q}}
the quantity you say is -k, not zero. It is a system with friction.
 
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anuttarasammyak said:
Say Force
\frac{\partial L}{\partial q}=-k \cdot{\dot{q}}
the quantity you say is -k, not zero. It is a system with friction.
But $$\frac{\partial L}{\partial q}=-k \cdot{\dot{q}}\neq \frac{\partial}{\partial q}\left(\frac{\partial L}{\partial \dot q}\right)$$
Sorry I should have indicated that it was a second derivative wrt a different var.
 
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Ya, I was wrong. Friction comes from another way.
 
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Leo Liu said:
Suppose the lagrangian of a system in generalized coordinates is ##L(q,\dot q,t)##. If the following expression arises in calculations ##\dfrac{\partial^2 L}{\partial q\partial \dot q}\,,## does it equal to 0? My reasoning is that since ##\dot q## and ##q## are functions of time, the expression above equals 0. Am I right? Thanks :)

In this context ##q## and ##\dot{q}## are not functions of time, rather they are simply the independent variables which make up ##q##-##\dot{q}## space. (They are only functions of time when evaluated on a solution to the equations of motion ##\boldsymbol{\gamma}(t) = (q(t), \dot{q}(t))##).

e.g. take the silly example ##L = q^2 \dot{q}##, then ##\dfrac{\partial^2 L}{\partial q\partial \dot q} = 2q##.
 
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ergospherical said:
e.g. take the silly example , then .
we can add the term ##2aq\dot{q}=\frac{d}{dt}(aq^2)## which does not change equation of motion, to Lagrangean. This term results
\frac{\partial^2 L}{\partial q \partial \dot{q}}=2a
 
what is your point? yes an equivalent lagrangian is ##\tilde{L} = q^2 \dot{q} + 2a q \dot{q}## and ##\dfrac{\partial^2 \tilde{L}}{\partial q \partial \dot{q}} = 2q + 2a##...
 
I meant adding that term to any normal Lagrangean, not to your example.

Anyway
q^2 \dot{q}+2aq\dot{q}=\frac{d}{dt}(\frac{q^3}{3}+aq^2)
This Lagrangean tells nothing to us.
 
I don't know what you are saying because it wasn't supposed to represent any physical system, it was just an arbitrary example to demonstrate the partial derivative
 
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I say adding any term of
\frac{d}{dt}f(q,t)
to Lagrangean does not harm it.
 
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  • #11
yes, but what has this got to do with the op?
 
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  • #12
I show a counter example to his
Leo Liu said:
Homework Statement:: .
Relevant Equations:: .

does it equal to 0?
for physical case.

e.g. a free particle
L=\frac{m}{2}\dot{q}^2 and,
L=\frac{m}{2}\dot{q}^2+2aq\dot{q} or
L=\frac{m}{2}\dot{q}^2+q^2\dot{q}+2aq\dot{q}
are equivalent in getting a solution. The latter Lanrangeans show a counter example to OP question.
 
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