Partial differentiation and explicit functions

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Discussion Overview

The discussion revolves around the nature of explicit functions in the context of partial differentiation, particularly focusing on the function f(x, t) = 6x + g(t), where g(t) is an arbitrary function of t. Participants explore the implications of this form on the partial derivative with respect to t and relate it to concepts in Lagrangian mechanics.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that f(x, t) is not an explicit function of t due to the presence of the x term, while others suggest that it is an explicit function of both x and t.
  • There is a challenge regarding the claim that ∂f/∂t = 0, with some arguing that f still depends on t unless g(t) is a constant.
  • One participant questions the behavior of ∂f/∂t when g(t) is an unknown arbitrary function, leading to the application of the chain rule to derive that ∂f/∂t = g'(t).
  • A participant raises a concern about a specific case in Lagrangian mechanics, questioning how ∂L/∂t can be zero when the Lagrangian includes a time derivative, while also being described as not an explicit function of time.
  • Another participant notes that the complexity of physical systems may lead to different interpretations, suggesting that the simplicity of examples can obscure more complicated scenarios.

Areas of Agreement / Disagreement

Participants express differing views on whether f(x, t) is an explicit function of t, and there is no consensus on the implications of this for the partial derivative ∂f/∂t. The discussion remains unresolved regarding the relationship between explicit functions and their derivatives in the context of Lagrangian mechanics.

Contextual Notes

Limitations include the dependence on the definitions of explicit functions and the specific forms of g(t). The discussion does not resolve how these definitions apply in more complex physical systems.

dyn
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Hi
For a function f ( x , t ) = 6x + g( t ) where g( t ) is an arbitrary function of t ; then is it correct to say that f ( x , t ) is not an explicit function of t ?

For the above function is it also correct that ∂f/∂t = 0 because f is not an explicit function of t ?

Thanks
 
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dyn said:
Hi
For a function f ( x , t ) = 6x + g( t ) where g( t ) is an arbitrary function of t ; then is it correct to say that f ( x , t ) is not an explicit function of t ?
I guess, yes, as long as the ##x## term is there. But this is more a matter of taste, I think than it is a rigor definition. But ##f(x,t)## is an explicit function of ##x## and ##t##.

If we had ##f(x)=g(t,x(t))## then ##f(x)## would not be an explicit function of ##t##.

dyn said:
For the above function is it also correct that ∂f/∂t = 0 because f is not an explicit function of t ?

Thanks

No. ##f## still depends on ##t##, except for the case ##g(t)=C## is a constant.
What do you get for ##\dfrac{\partial f}{\partial t}## if ##f(x,t)=6x+\sin(t)## ?
 
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Thanks. But what about the case where g ( t ) is an unknown arbitrary function ? What would ∂f/∂t be then ?
 
dyn said:
Thanks. But what about the case where g ( t ) is an unknown arbitrary function ? What would ∂f/∂t be then ?
Apply the chain rule. ##\partial_t f(x,t)=\partial_t(6x)+\partial_t g(t)=0+\partial_t g(t)=g'(t)##
 
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My question originally comes a question i am looking at regarding Lagrangian mechanics in cylindrical coordinates. The Lagrangian contains a term containing the time derivative of ρ but the book states that the Lagrangian is not an explicit function of time so ∂L/∂t = 0 and so the Hamiltonian is conserved..

I am confused about how ∂L/∂t = 0 when there is a time derivative in the Lagrangian and also L is said to be not an explicit function of time
 
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dyn said:
My question originally comes a question i am looking at regarding Lagrangian mechanics in cylindrical coordinates. The Lagrangian contains a term containing the time derivative of ρ but the book states that the Lagrangian is not an explicit function of time so ∂L/∂t = 0 and so the Hamiltonian is conserved..

I am confused about how ∂L/∂t = 0 when there is a time derivative in the Lagrangian and also L is said to be not an explicit function of time
I haven't said it is impossible. It depends on the functions involved. You gave a very simple example with separated variables. Physical systems are normally a lot more complicated.
 
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