20. Circular Motion
From Mechanics
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- | 20. Circular Motion | ||
- | Key Points | + | == '''Key Points''' == |
The diagram shows a particle | The diagram shows a particle | ||
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The position vector for the particle is: | The position vector for the particle is: | ||
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<math>\mathbf{r}=\left( r\cos \theta \right)\mathbf{i}+\left( r\sin \theta \right)\mathbf{j}</math> | <math>\mathbf{r}=\left( r\cos \theta \right)\mathbf{i}+\left( r\sin \theta \right)\mathbf{j}</math> | ||
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The particle has angular speed | The particle has angular speed | ||
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<math>t</math>: | <math>t</math>: | ||
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<math>\mathbf{r}=\left( r\cos \omega t \right)\mathbf{i}+\left( r\sin \omega t \right)\mathbf{j}</math> | <math>\mathbf{r}=\left( r\cos \omega t \right)\mathbf{i}+\left( r\sin \omega t \right)\mathbf{j}</math> | ||
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Differentiating the position vector gives the velocity: | Differentiating the position vector gives the velocity: | ||
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<math>\mathbf{v}=\left( -r\omega \sin \omega t \right)\mathbf{i}+\left( r\omega \cos \omega t \right)\mathbf{j}</math> | <math>\mathbf{v}=\left( -r\omega \sin \omega t \right)\mathbf{i}+\left( r\omega \cos \omega t \right)\mathbf{j}</math> | ||
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The magnitude of the velocity can now be found: | The magnitude of the velocity can now be found: | ||
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<math>\begin{align} | <math>\begin{align} | ||
& v=\sqrt{{{\left( -r\omega \sin \omega t \right)}^{2}}+{{\left( r\omega \cos \omega t \right)}^{2}}} \\ | & v=\sqrt{{{\left( -r\omega \sin \omega t \right)}^{2}}+{{\left( r\omega \cos \omega t \right)}^{2}}} \\ | ||
+ | & \\ | ||
& =\sqrt{{{r}^{2}}{{\omega }^{2}}({{\sin }^{2}}\omega t+{{\cos }^{2}}\omega t)} \\ | & =\sqrt{{{r}^{2}}{{\omega }^{2}}({{\sin }^{2}}\omega t+{{\cos }^{2}}\omega t)} \\ | ||
+ | & \\ | ||
& =\sqrt{{{r}^{2}}{{\omega }^{2}}} \\ | & =\sqrt{{{r}^{2}}{{\omega }^{2}}} \\ | ||
& =r\omega | & =r\omega | ||
\end{align}</math> | \end{align}</math> | ||
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The particle has speed, | The particle has speed, | ||
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Differentiating the velocity gives the acceleration: | Differentiating the velocity gives the acceleration: | ||
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<math>\begin{align} | <math>\begin{align} | ||
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& =-{{\omega }^{2}}\mathbf{r} | & =-{{\omega }^{2}}\mathbf{r} | ||
\end{align}</math> | \end{align}</math> | ||
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This shows that the acceleration has magnitude | This shows that the acceleration has magnitude | ||
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and | and | ||
<math>r.</math> | <math>r.</math> | ||
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<math>a=r{{\left( \frac{v}{r} \right)}^{2}}=\frac{{{v}^{2}}}{r}</math> | <math>a=r{{\left( \frac{v}{r} \right)}^{2}}=\frac{{{v}^{2}}}{r}</math> | ||
- | + | '''[[Example 20.1]]''' | |
- | Example 20.1 | + | |
A coin of mass 30 grams is placed on a turntable which rotates at 90 rpm. The coin is at a distance of 10 cm from the centre of the turntable. Find the magnitude of the coefficient of friction between the coin and the turntable, if the coin is on the point of slipping. | A coin of mass 30 grams is placed on a turntable which rotates at 90 rpm. The coin is at a distance of 10 cm from the centre of the turntable. Find the magnitude of the coefficient of friction between the coin and the turntable, if the coin is on the point of slipping. | ||
- | Solution | + | '''Solution''' |
The diagram shows the forces acting on the particle, its weight, the normal reaction from the surface and the friction. | The diagram shows the forces acting on the particle, its weight, the normal reaction from the surface and the friction. | ||
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[[Image:E20.1.GIF]] | [[Image:E20.1.GIF]] | ||
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The acceleration of | The acceleration of | ||
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The weight can be calculated first: | The weight can be calculated first: | ||
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<math>W=0.03\times 9.8=0.294\text{ N}</math> | <math>W=0.03\times 9.8=0.294\text{ N}</math> | ||
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As the vertical forces balance: | As the vertical forces balance: | ||
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<math>R=\text{ }0.\text{294 N}</math> | <math>R=\text{ }0.\text{294 N}</math> | ||
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The angular speed must be converted from rpm to | The angular speed must be converted from rpm to | ||
<math>\text{rad }{{\text{s}}^{-1}}</math>. | <math>\text{rad }{{\text{s}}^{-1}}</math>. | ||
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<math>\begin{align} | <math>\begin{align} | ||
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- | Example 20.2 | + | '''[[Example 20.2]]''' |
A car of mass 1200 kg travels round a bend with radius 20 metres at a constant speed of 12 <math>\text{m}{{\text{s}}^{-1}}</math>. Find the magnitude of the friction force acting on the car. Find the minimum possible value of the coefficient of friction between the tyres and the road. | A car of mass 1200 kg travels round a bend with radius 20 metres at a constant speed of 12 <math>\text{m}{{\text{s}}^{-1}}</math>. Find the magnitude of the friction force acting on the car. Find the minimum possible value of the coefficient of friction between the tyres and the road. | ||
- | Solution | + | '''Solution''' |
The diagram shows the forces acting on the car. | The diagram shows the forces acting on the car. | ||
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\end{align}</math> | \end{align}</math> | ||
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Resolving vertically: | Resolving vertically: | ||
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<math>R=1200\times 9.8=11760\text{ N}</math> | <math>R=1200\times 9.8=11760\text{ N}</math> | ||
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Then we can use the friction inequality | Then we can use the friction inequality | ||
<math>F\le mR</math>, to give, | <math>F\le mR</math>, to give, | ||
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<math>\begin{align} | <math>\begin{align} | ||
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& \mu \ge \text{0}\text{.735 (to 3 sf)} \\ | & \mu \ge \text{0}\text{.735 (to 3 sf)} \\ | ||
\end{align}</math> | \end{align}</math> | ||
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So the least value of | So the least value of | ||
<math>\mu </math> | <math>\mu </math> | ||
is 0.735. | is 0.735. |
Revision as of 11:25, 21 February 2010
Theory | Exercises |
Key Points
The diagram shows a particle
which moves with a circular path.
The position vector for the particle is:
rcos
i+
rsin
j
The particle has angular speed
If the particle is at
=
t
rcos
t
i+
rsin
t
j
Differentiating the position vector gives the velocity:
−r
sin
t
i+
r
cos
t
j
The magnitude of the velocity can now be found:
−r
sin
t
2+
r
cos
t
2=
r2
2(sin2
t+cos2
t)=
r2
2=r
The particle has speed,
Differentiating the velocity gives the acceleration:
−r
2cos
t
i+
−r
2sin
t
j=−
rcos
t
i+
rsin
t
j
=−
2r
This shows that the acceleration has magnitude
2
2
=rv
rv
2=rv2
A coin of mass 30 grams is placed on a turntable which rotates at 90 rpm. The coin is at a distance of 10 cm from the centre of the turntable. Find the magnitude of the coefficient of friction between the coin and the turntable, if the coin is on the point of slipping.
Solution
The diagram shows the forces acting on the particle, its weight, the normal reaction from the surface and the friction.
The acceleration of
The weight can be calculated first:
03
9
8=0
294 N
As the vertical forces balance:
294 N
The angular speed must be converted from rpm to
=90 rpm=6090
2
rad s-1=3
rad s-1
Using
2
03
0
1
(3
)2=0
267 N
Using
R
267=0
294
=0
2940
267=0
91 (to 2sf)
A car of mass 1200 kg travels round a bend with radius 20 metres at a constant speed of 12 \displaystyle \text{m}{{\text{s}}^{-1}}. Find the magnitude of the friction force acting on the car. Find the minimum possible value of the coefficient of friction between the tyres and the road.
Solution
The diagram shows the forces acting on the car.
Using \displaystyle F=ma radially, with \displaystyle a=\frac{{{v}^{2}}}{r} gives:
\displaystyle \begin{align} & F=1200\times \frac{{{12}^{2}}}{20}\text{ } \\ & =8640\text{ N} \end{align}
Resolving vertically:
\displaystyle R=1200\times 9.8=11760\text{ N}
Then we can use the friction inequality
\displaystyle F\le mR, to give,
\displaystyle \begin{align} & 8640\le \mu \times 11760 \\ & \mu \ge \frac{8640}{11760} \\ & \mu \ge \text{0}\text{.735 (to 3 sf)} \\ \end{align}
So the least value of \displaystyle \mu is 0.735.