Show that the vector \(f_{* x} v\) does not depend on the curve \(\boldsymbol{\varphi}\), but only on the vector \(\boldsymbol{v}\).

Short Answer

Expert verified
Based on the given solution, explain why the vector \(f_{*x}v\) is independent of the curve \(\boldsymbol{\varphi}\). The vector \(f_{*x}v\) is independent of the curve \(\boldsymbol{\varphi}\) because, when applying the pushforward on different curves, any differences in the resulting vectors were only related to the gradient operator \({\nabla}\) and the function \(f\). The pushforward did not directly depend on the curve \(\boldsymbol{\varphi}\) itself. Since it was not possible to attribute the differences in the pushforward of \(\boldsymbol{v}\) to the curves \(\boldsymbol{\varphi}_1\) and \(\boldsymbol{\varphi}_2\), it can be concluded that the vector \(f_{*x}v\) is indeed independent of the curve \(\boldsymbol{\varphi}\) and depends only on the vector \(\boldsymbol{v}\).

Step by step solution

01

Define the concepts

Let \(\boldsymbol{\varphi}\) be a curve and \(\boldsymbol{v}\) be a vector in tangent space \(T_x M\) at a point \(x\) on a manifold \(M\). Further, let \(f: M \to N\) be a smooth map between manifolds \(M\) and \(N\). Then, the pushforward \(f_{*x}v\) of the vector \(\boldsymbol{v}\) at point \(x\) is defined by the composition of maps \(f\) and \(d\boldsymbol{\varphi}\). To be more specific, $$ f_{*x}(\boldsymbol{v}) = df_{x}(\boldsymbol{v}) = (\boldsymbol{v} \cdot {\nabla})f $$ Where \(df_{x}\) is the differential of \(f\) at point \(x\) and \({\nabla}\) is the gradient operator.
02

Show that \(f_{*x}v\) is independent of the curve \(\boldsymbol{\varphi}\)

Now we need to show that the vector \(f_{*x}(\boldsymbol{v})\) depends only on the tangent vector \(\boldsymbol{v}\) and not on the curve \(\boldsymbol{\varphi}\). We'll prove this by contradiction. Suppose that there is a curve \(\boldsymbol{\varphi}_1\) and another curve \(\boldsymbol{\varphi}_2\) such that the pushforward of \(\boldsymbol{v}\) under \(f\) is different for each curve. That is, $$ f_{*x}(\boldsymbol{v}_{\boldsymbol{\varphi}_1}) \neq f_{*x}(\boldsymbol{v}_{\boldsymbol{\varphi}_2}). $$ Now consider a smooth function \(g: N \to \mathbb{R}\) on the manifold \(N\). Using the definition of the pushforward \(f_{*x}(\boldsymbol{v})\), we have $$ f_{*x}(\boldsymbol{v}_{\boldsymbol{\varphi}_1}) = (\boldsymbol{v}_{\boldsymbol{\varphi}_1} \cdot {\nabla})f $$ Similarly, for curve \(\boldsymbol{\varphi}_2\), $$ f_{*x}(\boldsymbol{v}_{\boldsymbol{\varphi}_2}) = (\boldsymbol{v}_{\boldsymbol{\varphi}_2} \cdot {\nabla})f $$ By our assumption, these two vectors are not equal. However, both vectors are only related to \(\boldsymbol{v}\) through the gradient operator \({\nabla}\) and function \(f\), and they do not directly depend on the curve \(\boldsymbol{\varphi}\) itself. This contradicts the assumption that \(f_{*x}(\boldsymbol{v}_{\boldsymbol{\varphi}_1})\) and \(f_{*x}(\boldsymbol{v}_{\boldsymbol{\varphi}_2})\) are different due to the curves \(\boldsymbol{\varphi}_1\) and \(\boldsymbol{\varphi}_2\). Therefore, we conclude that the vector \(f_{*x}v\) is indeed independent of the curve \(\boldsymbol{\varphi}\), and depends only on the vector \(\boldsymbol{v}\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

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.

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.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free