Chapter 4: Problem 2
Show that \(S O(3)\) is embedded in \(R^{9}\), and at the same time, that \(S O(3)\) is a manifold.
Chapter 4: Problem 2
Show that \(S O(3)\) is embedded in \(R^{9}\), and at the same time, that \(S O(3)\) is a manifold.
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Get started for freeExtend 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.
A rod of weight \(P\), tilted at an angle of \(60^{\circ}\) to the plane of a table, begins to fall with initial velocity zero (Figure 74). Find the constraint force of the table at the initial moment, considering the table as (a) absolutely smooth and (b) absolutely rough. (In the first case, the holonomic constraint holds the end of the rod on the plane of the table, and in the second case, at a given point.)
Show that the vector \(f_{* x} v\) does not depend on the curve \(\boldsymbol{\varphi}\), but only on the vector \(\boldsymbol{v}\).
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 $$ f_{*}: T M \Rightarrow T N \quad f_{*} v=f_{* x^{v}} \text { for } v \in T M_{*} $$
Suppose 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.
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