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Tush19
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how does the first step use mean value theorem? I don't get it , can anyone explain , thanks.
thanks but I couldn't find that mean value theorem statement anywhere ,all it shows that mean value theorem is the followingOrodruin said:The mean value theorem states that
$$
\int_x^{x+\delta x} f(s) ds = \delta x\, f(x^*)
$$
where ##x \leq x^* \leq x + \delta x##. Since ##f## is continuous, ##f(x^*) \to f(x)## for small ##\delta x##.
https://www.kristakingmath.com/blog/mean-value-theorem-for-integralsTush19 said:thanks but I couldn't find that mean value theorem statement anywhere ,all it shows that mean value theorem is the following
Wrong mean value theorem:Tush19 said:thanks but I couldn't find that mean value theorem statement anywhere ,all it shows that mean value theorem is the following
View attachment 295180
thank you so muchOrodruin said:Just to add: The mean value theorem for definite integrals is easy to obtain from the theorem you quoted. Just consider that
$$
(b-a) f’(c) = f(b) - f(a) = \int_a^b f’(x) dx
$$
and let ##g(x) = f’(x)##. You now have
$$
\int_a^b g(x) dx = (b-a) g(c)
$$
for some ##c## such that ##a\leq c\leq b##.
Noether's theorem is a fundamental principle in physics that states that for every continuous symmetry in a physical system, there is a corresponding conserved quantity. In other words, if a physical system remains unchanged under certain transformations, there will be a quantity that remains constant throughout the system's evolution.
Noether's theorem states that for every continuous symmetry, there is a conserved quantity. Time invariance is a type of symmetry, as a physical system should behave the same way regardless of when it is observed. Therefore, Noether's theorem can be applied to time invariance, resulting in a conserved quantity known as energy.
The mean value theorem is a mathematical concept that states that for a continuous function on a closed interval, there exists a point within that interval where the derivative of the function is equal to the average rate of change of the function over that interval. In Noether's theorem, the mean value theorem is used to show that the conserved quantity resulting from a symmetry is equal to the average value of the corresponding Lagrangian over a specific interval of time.
Yes, Noether's theorem can be applied to all physical systems that exhibit continuous symmetries. This includes classical mechanics, electromagnetism, and quantum mechanics.
Noether's theorem has been applied in various fields of physics, including classical mechanics, quantum mechanics, and general relativity. It has also been used in the study of particle physics and cosmology. Additionally, Noether's theorem has been used to explain the conservation of energy, momentum, and angular momentum in physical systems.