Chapter 4: Problem 3
Show that the vector \(f_{* x} v\) does not depend on the curve \(\boldsymbol{\varphi}\), but only on the vector \(\boldsymbol{v}\).
Chapter 4: Problem 3
Show that the vector \(f_{* x} v\) does not depend on the curve \(\boldsymbol{\varphi}\), but only on the vector \(\boldsymbol{v}\).
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Get started for freeSuppose that a rigid body is moving under its own inertia. Show that its center of mass moves linearly and uniformly. If the center of mass is at rest, then the angular momentum with respect to it is conserved.
Let \(\mathbf{x}=\left(x_{1}, \ldots, x_{m}\right)\) be coordinates in a neighborhood of \(\mathbf{x} \in M\), and \(\mathbf{y}=\left(y_{1} \ldots, y_{n}\right)\) be coordinates in a neighborhood of \(\mathrm{y} \in N\), Let \(\xi\) be the set of components of the vector \(v_{\text {, and }}\) \(\eta\) the set of components of the vector \(f_{* x}\). Show that $$ \boldsymbol{\eta}=\frac{\partial \mathbf{y}}{\partial \mathbf{x}} \xi \text {. i.e.. } n_{i}=\sum_{j} \frac{\partial y_{i}}{\partial x_{j}} \xi_{j} . $$ Taking the union of the mappings \(f_{e x}\) for all \(x\), we get a mapping of the whole tangent bundle $$ f_{*}: T M \Rightarrow T N \quad f_{*} v=f_{* x^{v}} \text { for } v \in T M_{*} $$
Extend Noether's theorem to non-autonomous lagrangian systems. Hint. Let \(M_{1}=M \times \mathbb{R}\) be the extended configuration space (the direct product of the configuration manifold \(M\) with the time axis \(\mathbb{R}\) ). Define a function \(L_{1}: T M_{1} \rightarrow \mathbb{R}\) by $$ L \frac{d t}{d z} \text { : } $$ i.e., in lucal coordinates \(q, t\) on \(M_{1}\) we define it by the formula $$ L_{1}\left(\mathbf{q}, t, \frac{d \mathbf{q}}{d \tau}, \frac{d t}{d \tau}\right)=L\left(\mathbf{q}, \frac{d \mathbf{q} / d \tau}{d t, d \tau}, t\right) \frac{d t}{d \tau} $$ We apply Noether's theorem to the lagrangian system \(\left(M_{2}, L_{1}\right)\). If \(L_{1}\) admits the transformations \(h^{s}: M_{1} \rightarrow M_{1}\). we obtain a first integral \(l_{1}: T M_{1} \rightarrow \mathbb{R}\). Since \(\int L d t=\int L_{1} d \tau_{\text {. this reduces }}\) to a first integral \(I: T M \times\) of \(\rightarrow \mathbb{R}\) of the viginal system. If. in local coordinates \((\boldsymbol{q}, t)\) on \(M_{1}\), we have \(I_{1}=I_{1}(\mathbf{q}, t, d \mathbf{q} / d \tau, d l / d \tau)\), then \(I(\mathbf{q}, \mathbf{q}, t)=l_{1}\left(\mathbf{q}, I_{1}, \dot{\mathbf{q}}, 1\right)\). In particular, if \(L\) does not depend on time, \(L_{1}\) admits translations along time, \(h^{s}(q, t)=\) (q. \(t+5\) ). The corresponding first integral \(l\) is the energy integral.
Show that \(S O(3)\) is embedded in \(R^{9}\), and at the same time, that \(S O(3)\) is a manifold.
Suppose that a particle moves in the field of the uniform helical line \(x=\cos \varphi\). \(y=\sin \varphi_{z} z=c \varphi\). Find the law of conservation corresponding to this helical symmetry.
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