How can you explain $cot(alpha)= dfrac{d}{dtheta}cdot ln(r) = dfrac{1}{r} dfrac{dr}{dt}$ in a polar...
This alinea is about the $$cot(alpha)= dfrac{d}{dtheta}cdot ln(r) = dfrac{1}{r} dfrac{dr}{dt}.$$ Where does the $ln (r)$ come from? How can you derive it from that picture? I want to use that for the $$nabla f(r,theta)= dfrac {partial f}{partial r}vec e_r + dfrac {1}{r}dfrac{partial f}{partial theta}vec e_theta.$$ I know what the definition is of the gradient (i.e. it's a partial derivative of the function with respect to every component in a particular dimension for my case $x,y,z$). The only thing is that I don't know how to convert that to polar coordinates. Can someone please clarify this?
EDIT: I know that the derivative of $ln(x)= 1/x$. So bringing in $ln r$ would be convenient.
coordinate-systems derivatives
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This question came from our site for active researchers, academics and students of physics.
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This alinea is about the $$cot(alpha)= dfrac{d}{dtheta}cdot ln(r) = dfrac{1}{r} dfrac{dr}{dt}.$$ Where does the $ln (r)$ come from? How can you derive it from that picture? I want to use that for the $$nabla f(r,theta)= dfrac {partial f}{partial r}vec e_r + dfrac {1}{r}dfrac{partial f}{partial theta}vec e_theta.$$ I know what the definition is of the gradient (i.e. it's a partial derivative of the function with respect to every component in a particular dimension for my case $x,y,z$). The only thing is that I don't know how to convert that to polar coordinates. Can someone please clarify this?
EDIT: I know that the derivative of $ln(x)= 1/x$. So bringing in $ln r$ would be convenient.
coordinate-systems derivatives
migrated from physics.stackexchange.com Dec 26 at 12:07
This question came from our site for active researchers, academics and students of physics.
1
I'm voting to move this to Mathematics SE
– Aaron Stevens
Dec 26 at 1:08
add a comment |
This alinea is about the $$cot(alpha)= dfrac{d}{dtheta}cdot ln(r) = dfrac{1}{r} dfrac{dr}{dt}.$$ Where does the $ln (r)$ come from? How can you derive it from that picture? I want to use that for the $$nabla f(r,theta)= dfrac {partial f}{partial r}vec e_r + dfrac {1}{r}dfrac{partial f}{partial theta}vec e_theta.$$ I know what the definition is of the gradient (i.e. it's a partial derivative of the function with respect to every component in a particular dimension for my case $x,y,z$). The only thing is that I don't know how to convert that to polar coordinates. Can someone please clarify this?
EDIT: I know that the derivative of $ln(x)= 1/x$. So bringing in $ln r$ would be convenient.
coordinate-systems derivatives
This alinea is about the $$cot(alpha)= dfrac{d}{dtheta}cdot ln(r) = dfrac{1}{r} dfrac{dr}{dt}.$$ Where does the $ln (r)$ come from? How can you derive it from that picture? I want to use that for the $$nabla f(r,theta)= dfrac {partial f}{partial r}vec e_r + dfrac {1}{r}dfrac{partial f}{partial theta}vec e_theta.$$ I know what the definition is of the gradient (i.e. it's a partial derivative of the function with respect to every component in a particular dimension for my case $x,y,z$). The only thing is that I don't know how to convert that to polar coordinates. Can someone please clarify this?
EDIT: I know that the derivative of $ln(x)= 1/x$. So bringing in $ln r$ would be convenient.
coordinate-systems derivatives
coordinate-systems derivatives
edited Dec 26 at 12:25
Bernard
118k639112
118k639112
asked Dec 25 at 20:24
Anonymous I
8302826
8302826
migrated from physics.stackexchange.com Dec 26 at 12:07
This question came from our site for active researchers, academics and students of physics.
migrated from physics.stackexchange.com Dec 26 at 12:07
This question came from our site for active researchers, academics and students of physics.
1
I'm voting to move this to Mathematics SE
– Aaron Stevens
Dec 26 at 1:08
add a comment |
1
I'm voting to move this to Mathematics SE
– Aaron Stevens
Dec 26 at 1:08
1
1
I'm voting to move this to Mathematics SE
– Aaron Stevens
Dec 26 at 1:08
I'm voting to move this to Mathematics SE
– Aaron Stevens
Dec 26 at 1:08
add a comment |
2 Answers
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The “physics-y” way to do this is to consider $P$ as the position of a particle moving along the curve $K$. If $mathbf{r}$ is its position vector from $O$ to $P$, then $alpha$ is the angle between its velocity vector $dot{mathbf{r}}$ (along the tangent line $t$) and the position vector $mathbf{r}$. So
$$cos{alpha}=frac{dot{mathbf{r}}}{|dot{mathbf{r}}|}cdotfrac{mathbf{r}}{|mathbf{r}|}$$
In polar coordinates, the position vector is
$$mathbf{r}=rhat{mathbf{r}}.$$
Differentiating it with respect to time gives the velocity vector
$$dot{mathbf{r}}=dot{r}hat{mathbf{r}}+rdot{hat{mathbf{r}}}=dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}.$$
Thus we have
$$cos{alpha}=frac{dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}}{|dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}|}cdothat{mathbf{r}}=frac{dot{r}}{sqrt{dot{r}^2+r^2dot{theta}^2}}$$
which implies
$$cot{alpha}=frac{dot{r}}{rdot{theta}}=frac{1}{r}frac{dr}{dtheta}=frac{d}{dtheta}ln{r}.$$
Thx. That refers to a textbook I've found.
– Anonymous I
Dec 25 at 23:05
add a comment |
I like this solution
How can you derivate it from this picture

Nice answer, it's simple and useful. But please, you should not post formulae in pictures. Type them instead using Mathjax. There are many reasons, including optimisation of algorithms and helping users whose device doesn't display them well.
– FGSUZ
Dec 26 at 10:11
add a comment |
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2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
The “physics-y” way to do this is to consider $P$ as the position of a particle moving along the curve $K$. If $mathbf{r}$ is its position vector from $O$ to $P$, then $alpha$ is the angle between its velocity vector $dot{mathbf{r}}$ (along the tangent line $t$) and the position vector $mathbf{r}$. So
$$cos{alpha}=frac{dot{mathbf{r}}}{|dot{mathbf{r}}|}cdotfrac{mathbf{r}}{|mathbf{r}|}$$
In polar coordinates, the position vector is
$$mathbf{r}=rhat{mathbf{r}}.$$
Differentiating it with respect to time gives the velocity vector
$$dot{mathbf{r}}=dot{r}hat{mathbf{r}}+rdot{hat{mathbf{r}}}=dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}.$$
Thus we have
$$cos{alpha}=frac{dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}}{|dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}|}cdothat{mathbf{r}}=frac{dot{r}}{sqrt{dot{r}^2+r^2dot{theta}^2}}$$
which implies
$$cot{alpha}=frac{dot{r}}{rdot{theta}}=frac{1}{r}frac{dr}{dtheta}=frac{d}{dtheta}ln{r}.$$
Thx. That refers to a textbook I've found.
– Anonymous I
Dec 25 at 23:05
add a comment |
The “physics-y” way to do this is to consider $P$ as the position of a particle moving along the curve $K$. If $mathbf{r}$ is its position vector from $O$ to $P$, then $alpha$ is the angle between its velocity vector $dot{mathbf{r}}$ (along the tangent line $t$) and the position vector $mathbf{r}$. So
$$cos{alpha}=frac{dot{mathbf{r}}}{|dot{mathbf{r}}|}cdotfrac{mathbf{r}}{|mathbf{r}|}$$
In polar coordinates, the position vector is
$$mathbf{r}=rhat{mathbf{r}}.$$
Differentiating it with respect to time gives the velocity vector
$$dot{mathbf{r}}=dot{r}hat{mathbf{r}}+rdot{hat{mathbf{r}}}=dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}.$$
Thus we have
$$cos{alpha}=frac{dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}}{|dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}|}cdothat{mathbf{r}}=frac{dot{r}}{sqrt{dot{r}^2+r^2dot{theta}^2}}$$
which implies
$$cot{alpha}=frac{dot{r}}{rdot{theta}}=frac{1}{r}frac{dr}{dtheta}=frac{d}{dtheta}ln{r}.$$
Thx. That refers to a textbook I've found.
– Anonymous I
Dec 25 at 23:05
add a comment |
The “physics-y” way to do this is to consider $P$ as the position of a particle moving along the curve $K$. If $mathbf{r}$ is its position vector from $O$ to $P$, then $alpha$ is the angle between its velocity vector $dot{mathbf{r}}$ (along the tangent line $t$) and the position vector $mathbf{r}$. So
$$cos{alpha}=frac{dot{mathbf{r}}}{|dot{mathbf{r}}|}cdotfrac{mathbf{r}}{|mathbf{r}|}$$
In polar coordinates, the position vector is
$$mathbf{r}=rhat{mathbf{r}}.$$
Differentiating it with respect to time gives the velocity vector
$$dot{mathbf{r}}=dot{r}hat{mathbf{r}}+rdot{hat{mathbf{r}}}=dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}.$$
Thus we have
$$cos{alpha}=frac{dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}}{|dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}|}cdothat{mathbf{r}}=frac{dot{r}}{sqrt{dot{r}^2+r^2dot{theta}^2}}$$
which implies
$$cot{alpha}=frac{dot{r}}{rdot{theta}}=frac{1}{r}frac{dr}{dtheta}=frac{d}{dtheta}ln{r}.$$
The “physics-y” way to do this is to consider $P$ as the position of a particle moving along the curve $K$. If $mathbf{r}$ is its position vector from $O$ to $P$, then $alpha$ is the angle between its velocity vector $dot{mathbf{r}}$ (along the tangent line $t$) and the position vector $mathbf{r}$. So
$$cos{alpha}=frac{dot{mathbf{r}}}{|dot{mathbf{r}}|}cdotfrac{mathbf{r}}{|mathbf{r}|}$$
In polar coordinates, the position vector is
$$mathbf{r}=rhat{mathbf{r}}.$$
Differentiating it with respect to time gives the velocity vector
$$dot{mathbf{r}}=dot{r}hat{mathbf{r}}+rdot{hat{mathbf{r}}}=dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}.$$
Thus we have
$$cos{alpha}=frac{dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}}{|dot{r}hat{mathbf{r}}+rdot{theta}hat{mathbf{theta}}|}cdothat{mathbf{r}}=frac{dot{r}}{sqrt{dot{r}^2+r^2dot{theta}^2}}$$
which implies
$$cot{alpha}=frac{dot{r}}{rdot{theta}}=frac{1}{r}frac{dr}{dtheta}=frac{d}{dtheta}ln{r}.$$
answered Dec 25 at 22:14
G. Smith
2213
2213
Thx. That refers to a textbook I've found.
– Anonymous I
Dec 25 at 23:05
add a comment |
Thx. That refers to a textbook I've found.
– Anonymous I
Dec 25 at 23:05
Thx. That refers to a textbook I've found.
– Anonymous I
Dec 25 at 23:05
Thx. That refers to a textbook I've found.
– Anonymous I
Dec 25 at 23:05
add a comment |
I like this solution
How can you derivate it from this picture

Nice answer, it's simple and useful. But please, you should not post formulae in pictures. Type them instead using Mathjax. There are many reasons, including optimisation of algorithms and helping users whose device doesn't display them well.
– FGSUZ
Dec 26 at 10:11
add a comment |
I like this solution
How can you derivate it from this picture

Nice answer, it's simple and useful. But please, you should not post formulae in pictures. Type them instead using Mathjax. There are many reasons, including optimisation of algorithms and helping users whose device doesn't display them well.
– FGSUZ
Dec 26 at 10:11
add a comment |
I like this solution
How can you derivate it from this picture

I like this solution
How can you derivate it from this picture

answered Dec 26 at 8:35
Eli
1212
1212
Nice answer, it's simple and useful. But please, you should not post formulae in pictures. Type them instead using Mathjax. There are many reasons, including optimisation of algorithms and helping users whose device doesn't display them well.
– FGSUZ
Dec 26 at 10:11
add a comment |
Nice answer, it's simple and useful. But please, you should not post formulae in pictures. Type them instead using Mathjax. There are many reasons, including optimisation of algorithms and helping users whose device doesn't display them well.
– FGSUZ
Dec 26 at 10:11
Nice answer, it's simple and useful. But please, you should not post formulae in pictures. Type them instead using Mathjax. There are many reasons, including optimisation of algorithms and helping users whose device doesn't display them well.
– FGSUZ
Dec 26 at 10:11
Nice answer, it's simple and useful. But please, you should not post formulae in pictures. Type them instead using Mathjax. There are many reasons, including optimisation of algorithms and helping users whose device doesn't display them well.
– FGSUZ
Dec 26 at 10:11
add a comment |
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I'm voting to move this to Mathematics SE
– Aaron Stevens
Dec 26 at 1:08