Math, asked by gshivani9991, 9 months ago

A particle describes the curve r = ae^theta with constant angular velocity. Show
that its radial acceleration is zero and the transverse acceleration varies as its
distance from the pole.

Answers

Answered by pulakmath007
8

SOLUTION

TO PROVE

A particle describes the curve \displaystyle\sf{ \:r = a \:  {e}^{ \theta}  } with constant angular velocity. Show that its radial acceleration is zero and the transverse acceleration varies as it's distance from the pole.

EVALUATION

Here the given curve is

\displaystyle\sf{ \:r = a \:  {e}^{ \theta}  }

Now

\displaystyle\sf{ Angular  \: Velocity  =  \frac{d\theta}{dt}  =  \omega  = constant  }

Here

\displaystyle\sf{ \:r = a \:  {e}^{ \theta}  }

\displaystyle\sf{ \implies \: \frac{dr}{dt}  = a \:  {e}^{ \theta}   \frac{d\theta}{dt}  = r \omega}

\displaystyle\sf{ \therefore \: \frac{ {d}^{2} r}{d {t}^{2} }  =\omega  \frac{dr}{dt}  =\omega. r \omega =  {\omega}^{2}r}

∴ Radial acceleration

 \sf{ = f_r}

\displaystyle\sf{  =  \frac{ {d}^{2} r}{d {t}^{2} }  - r {\bigg( \frac{dr}{dt}  \bigg) }^{2}  }

\displaystyle\sf{   =  {\omega}^{2}r - r{\omega}^{2}}

 = 0

∴ Transverse acceleration

 \sf{ = f_{ \theta} }

\displaystyle\sf{  =  \frac{1}{r}  \frac{d}{dt}   \bigg( {r}^{2}   \frac{d\theta}{dt}   \bigg)}

\displaystyle\sf{  =  \frac{1}{r}  \frac{d}{dt}   \bigg( {r}^{2}    \omega  \bigg)}

\displaystyle\sf{  =  \frac{  \omega }{r}  \frac{d}{dt}   \bigg( {r}^{2}  \bigg)}

\displaystyle\sf{  =  \frac{  \omega }{r} .2r \frac{dr}{dt} }

\displaystyle\sf{  =  \frac{  \omega }{r} .2r .r   \omega }

\displaystyle\sf{  =2 {\omega}^{2} r }

\displaystyle\sf{ \therefore \:  \: f_{ \theta} =2 {\omega}^{2} r }

\displaystyle\sf{ \therefore \:  \: f_{ \theta}  \propto \:  r }

∴ Radial acceleration = 0

\displaystyle\sf{ \therefore \:  \: Transverse  \:  \: acceleration    \propto \:  r }

Hence radial acceleration is zero and the transverse acceleration varies as it's distance from the pole.

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