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From material derivatives to partial derivatives in the wave equation

It happens that the convective term $\mathbf{\dot x}\cdot \nabla \mathbf u$ describes the transport of the field $\mathbf u$ over the flow, but in waves there is no transport of matter. Another way to ...
Ruffolo's user avatar
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Why must the total time derivative only be a linear function of velocity?

It comes down to how the differentiation works. The function I mentioned, $f(q, t)=q^2$ would indeed be a linear function once differentiated: $$\frac{d}{dt}(q^2)=\frac{d}{dt}(q\cdot q)$$ Which, when ...
Kyle Tennison's user avatar
0 votes

Why must the total time derivative only be a linear function of velocity?

The Taylor expansion is: $f(x+\delta)=f(x)+f'(x)\delta+...$ Here $x=v^2$, and you know that $v^2+\delta=(\vec{v}+\vec{\epsilon})^2=v^2+2\vec{v}.\vec{\epsilon}+\epsilon^2$ thus, $\delta=2\vec{v}.\vec{\...
Pato Galmarini's user avatar
2 votes
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Covariant derivative acting on Dirac delta function

Let's be a bit systematic. Let $M$ be a smooth $m$-dimensional manifold. Suppose that $M$ is orientable and oriented (so that we can use $m$-forms as densities). Let $\xi:E\rightarrow M$ be a smooth ...
Bence Racskó's user avatar
3 votes

Clarification of Ehrenfest theorem

The Newton's equation of motion in potential $V(x)$ are: $$ \dot{x}=\frac{p}{m},\dot{p}=-\frac{dV(x)}{dx} $$ or simply $$m\ddot{x}=-\frac{dV(x)}{dx}=F(x),$$ where $F(x)= -\frac{dV(x)}{dx}$ is called (...
Roger V.'s user avatar
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Arguing that the time derivative of $\exp(-iHt)$ is $-iH\exp(-iHt)$ without taylor expansion

But I cannot see how I can ignore the eigenvectors as if they do not exist and use chain rule Do you want to prove it without using the spectrum or Taylor expansion? Let $U(t) = e^{-iHt}$. By ...
Ruffolo's user avatar
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0 votes

Arguing that the time derivative of $\exp(-iHt)$ is $-iH\exp(-iHt)$ without taylor expansion

If $H$ is a hermitian matrix with eigenvectors $$H|n\rangle=\epsilon_n|n\rangle,$$ (note that the eigenvectors and eigenvalues do not depend on time) then we could write $$ H= \sum_n|n\rangle\langle n|...
Roger V.'s user avatar
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Arguing that the time derivative of $\exp(-iHt)$ is $-iH\exp(-iHt)$ without taylor expansion

Since the Hamiltonian is a self-adjoint operator, you can use the spectral theorem to write $$H = \int_\mathbb{R} \lambda \, dP_\lambda.$$ Then, as the exponential is a measurable function, $$ \exp(-...
Apoorv Potnis's user avatar
4 votes
Accepted

Understanding the definition of the covariant derivative

In the case of a scalar field, the covariant derivative equals the partial derivative. In the case of a tensor field of higher rank, there are further terms involving connection coefficients: for rank ...
Andrew Steane's user avatar
3 votes

Understanding the definition of the covariant derivative

The covariant derivative of a covector field $V_\mu$ is: $$ V_{\mu;\nu} = V_{\mu,\nu} - \Gamma^\lambda{}_{\mu\nu} V_{\lambda} $$ The covariant derivative of a scalar field is just its partial ...
Amit's user avatar
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3 votes
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Need help in understanding Tangential Acceleration

Derivatives speak to the instantaneous behavior at a point. It is possible to have a 1st derivative that is non-zero and a 2nd derivative that is 0 at a point. They're simply measuring two different ...
Cort Ammon's user avatar
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0 votes

"Deriving" the covariant derivative

I think you just need to find an operator $D_{\mu}$ such that $$ D'_{\mu}\phi' = e^{i\beta}D_{\mu}\phi. $$ For some arbitrary phase $\beta$. The normal derivative is a starting point. $$ \partial_{\mu}...
Ruffolo's user avatar
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1 vote

Derivative for the Maxwell field

$$\frac{\partial(\partial_{\mu}A^{\sigma})}{\partial(\partial^{\nu}A_{\lambda})}$$ I can't understand whether I must raise the lower index of the partial derivative, and lower the one of the vector ...
hft's user avatar
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3 votes

The definition of the Lie Derivative

It's just because you want to compare two objects at the same point. In differential geometry you can NOT compare objects at different points since they live in different spaces. The pull back allows ...
Filippo's user avatar
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1 vote

Why are Weyl's Equations composed of only first-order derivatives?

Equations 2nd-order in time (like the Klein-Gordon Equation) yield negative energy solutions which are not consistent if interpreted as wave functions of physical particles (as Schroedinger and Dirac ...
bapowell's user avatar
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3 votes

Is it ever possible that the object is moving with a velocity such that its rate of change of speed is not constant but acceleration is constant?

In general if $v$ denotes the velocity, the rate of change of speed is \begin{align*}\frac{\text{d}|v|}{\text{d}t} &= \frac{\text{d}}{\text{d}t} \sqrt{ \left< v, v \right> } \\&= \frac{1}...
Adayah's user avatar
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6 votes

Is it ever possible that the object is moving with a velocity such that its rate of change of speed is not constant but acceleration is constant?

Yes, this happens all the time. Fire a gun, or throw a ball, or do just about anything that involves making something move. And ignore things like air resistance, curvature of the earth and so on. ...
Dawood ibn Kareem's user avatar
9 votes

Is it ever possible that the object is moving with a velocity such that its rate of change of speed is not constant but acceleration is constant?

Prelude - a (hopefully) fun but counterintuitive geometrical fact A nice fact which may be a bit counterintuitive, is that if you have a square with diagonal length $\ell$ and this length varies in ...
Amit's user avatar
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26 votes

Is it ever possible that the object is moving with a velocity such that its rate of change of speed is not constant but acceleration is constant?

Hint: In the projectile motion (without drag) the acceleration $\vec{a}=\frac{d\vec{v}}{dt}$ is constant. However $\frac{d|\vec{v}|}{dt}$ is not constant, since it is negative when the projectile is ...
Qmechanic's user avatar
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