Deriving the Differential Position Vector in Cylindrical Coordinates

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Homework Help Overview

The discussion revolves around deriving the differential position vector in cylindrical coordinates, specifically examining the expression $$\mathrm dr=\hat r \mathrm dr + r \hat \theta \mathrm d \theta + \hat k \mathrm dz$$ and its relation to the kinetic energy equation $$T=\frac{1}{2}m[\dot{x}^2+(r\dot{\theta})^2]$$.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the derivation of the differential position vector, with some suggesting geometric or algebraic methods for understanding the expression. Questions arise regarding the notation used and the relationship between the components of the position vector.

Discussion Status

Participants are actively exploring the derivation process and clarifying notation. Some have noted discrepancies in the representation of the position vector, while others are considering how to properly express the differential changes in cylindrical coordinates.

Contextual Notes

There are mentions of confusion regarding the notation for the position vector and its components, as well as the implications of using different symbols for similar concepts in cylindrical coordinates.

Istiak
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Homework Statement
differential position vector
Relevant Equations
vectors, differentiation
I had an equation. $$T=\frac{1}{2}m[\dot{x}^2+(r\dot{\theta})^2]$$ Then, they wrote that $$\mathrm dr=\hat r \mathrm dr + r \hat \theta \mathrm d \theta + \hat k \mathrm dz$$ I was thinking how they had derived it. The equation is looking like, they had differentiate "something". Is it just an equation which came from logic and mind rather than deriving?
 
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Istiakshovon said:
Homework Statement:: differential position vector
Relevant Equations:: vectors, differentiation

I had an equation. $$T=\frac{1}{2}m[\dot{x}^2+(r\dot{\theta})^2]$$ Then, they wrote that $$\mathrm dr=\hat r \mathrm dr + r \hat \theta \mathrm d \theta + \hat k \mathrm dz$$ I was thinking how they had derived it. The equation is looking like, they had differentiate "something". Is it just an equation which came from logic and mind rather than deriving?
This is very similar to the question you asked previously about cylindrical coordinates. You should be able to derive that expression either geometrically (by drawing a diagram) or algebraically (by converting from Cartesian).
 
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PeroK said:
This is very similar to the question you asked previously about cylindrical coordinates. You should be able to derive that expression either geometrically (by drawing a diagram) or algebraically (by converting from Cartesian).
What I could draw that is It :

1630511980943.png

I think it wasn't correct graph. 🤔 (cylindrical was little bit harder that's why I am not taking a look at that.)
 
Ow! I got a figure in book.

Screenshot from 2021-09-01 19-07-53.png
 
Istiakshovon said:
Then, they wrote that $$\mathrm dr=\hat r \mathrm dr + r \hat \theta \mathrm d \theta + \hat k \mathrm dz$$
This is the differential increment in the position vector: How a small change in ##\vec r## relates to small changes in ##r, \theta, z##.

Note that it should be ##d\vec r## on the left hand side.
 
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PeroK said:
This is the differential increment in the position vector: How a small change in ##\vec r## relates to small changes in ##r, \theta, z##.

Note that it should be ##d\vec r## on the left hand side.
got the answer... But, book wrote that; that's dr on the LHS.
 
Istiakshovon said:
got the answer... But, book wrote that; that's dr on the LHS.
The RHS is a vector, so the LHS must be too.
 
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Yes the differential position vector comes from the derivative (with respect to time) of the position vector.
The position vector in cylindrical coordinates is $$\vec{r}=r(t)\hat r(t)+z(t)\hat z$$.

Take the derivative of that with respect to time and have in mind that ##\hat r(t)=\cos\theta(t)\hat x+\sin\theta(t)\hat y##. Also have in mind that ##r'(t)dt=dr,\theta'(t)dt=d\theta,z'(t)dt=dz## and that the unit vector ##\hat \theta(t)=-\sin\theta(t)\hat x+\cos\theta(t)\hat y##.
 
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Ah btw, I found a mini problem both with the OP notation and mine notation at post #8, we use the same letter ##r## to denote the position vector and the radius in cylindrical coordinates, i should 've written $$\vec{r}=\rho(t)\hat \rho(t)+z(t)\hat z$$, and the OP I think should write $$d\vec{r}=d\rho\hat\rho+\rho d\theta\hat\theta+dz\hat z$$
 

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