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Calculate the potential and the intensity of the gravitational field at a distance $x> 0$ in the axis of thin homogeneous circular plate of radius $a$ and mass $M$.

enter image description here

Could anybody describe how to calculate this? Slowly and in detail. I'm helpless.

Answer is: potencial $\phi = - \frac {2 \kappa M}{a^2}(\sqrt{a^2+x^2}-x)$ and intesity $K = \frac {2 \kappa M}{a^2} \left( \frac{x}{\sqrt{a^2+x^2}}-1 \right)$

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If anybody finds this question incomprehensible, please, leave a comment, I will try to rewrite it. I'm not a native speaker, so I might do some mistakes. –  user50222 Apr 29 '13 at 9:32
    
first find out for a ring. then add for infinite rings that form a disc using integration. –  Mr.ØØ7 Apr 29 '13 at 17:56
    
How to do that? I can't find any example. –  user50222 Apr 29 '13 at 20:58
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2 Answers

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First let us calculate the potential for a ring of radius $a$ at a distance $x$ from the center along the axis

Potential due to an infinitesimal mass element $dm$ will be $$\frac{-Gdm}{\sqrt{a^2+x^2}}$$

Potential due to the ring is then $$\int{\frac{-Gdm}{\sqrt{a^2+x^2}}}=\frac{-G}{\sqrt{a^2+x^2}}\int{dm}=\frac{-Gm}{\sqrt{a^2+x^2}}$$

Since $G, a, x$ are constant

Now let us break the disc into infinitesimal rings of mass $dm=2\pi rdr\frac{M}{\pi a^2} (=area * density)$

The potential due to a ring of radius $r$ and mass $dm$ as given above is $$\frac{-Gdm}{\sqrt{r^2+x^2}}=\frac{-2GMrdr}{a^2\sqrt{r^2+x^2}}$$

Integrating this from $0$ to $a$ $$\int{\frac{-2GMrdr}{a^2\sqrt{r^2+x^2}}}$$ $$=\frac{-GM}{a^2}\int{\frac{2rdr}{\sqrt{r^2+x^2}}}$$ putting $t^2=r^2+a^2$ and $2rdr=2tdt$ $$=\frac{-GM}{a^2}\int{\frac{2tdt}{\sqrt{t^2}}}$$ $$=\frac{-GM}{a^2}[2t]^{\sqrt{a^2+x^2}}_{x}$$ $$=\frac{-2GM}{a^2}({\sqrt{a^2+x^2}}-{x})$$

For intensity, it can be seen by symmetry that it is along the axis thus we work only with axial components

So, for ring $$\int\frac{-Gdmcos\theta}{a^2+x^2}$$ where $\theta$ is half of the angle subtented by the point on the ring $$cos\theta=\frac{x}{\sqrt{a^2+x^2}}$$

$$K=\int\frac{-Gxdm}{(a^2+x^2)^{3/2}}=\frac{-Gxm}{(a^2+x^2)^{3/2}}$$

For a disc, based on the same reasoning as in potential, it is

$$K=\int\frac{-Gxdm}{(r^2+x^2)^{3/2}}$$ $$=\int\frac{-2GMxrdr}{a^2(r^2+x^2)^{3/2}}$$ $$=\int\frac{-2GMxtdt}{a^2(t^2)^{3/2}}$$ $$=\int\frac{-2GMxdt}{a^2t^2}$$ $$=\frac{-2GMx}{a^2}[\frac{-1}{t}]^{\sqrt{a^2+x^2}}_x$$

$$K=\frac {2 G M}{a^2} \left( \frac{x}{\sqrt{a^2+x^2}}-1 \right)$$

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Let's break the disc into small rings,enter image description here

Here the mass in the disc is at a same distance $\sqrt{x^2+r^2}$ from the axis point A.

So, potential $$dE=-\dfrac{G.dm}{\sqrt{x^2+r^2}}$$

Where $dm$= mass of the ring. So, $$dm=2\pi r.dr \times \dfrac{M}{\pi R^2}$$

Also $r=xtan\phi$ , so $dr=x\sec^2\phi. d\phi$

So, the potential is $$dP=-\dfrac{GM.2\pi x\tan\phi x\sec^2\phi.d\phi}{(x\sqrt{1+\tan^2\phi})\times \pi R^2}=-\dfrac{2 GMx}{R^2}\times tan\phi.\sec\phi.d\phi$$

. So, $$P=-\dfrac{2GMx}{R^2}\times \int_0^{\tan^{-1}R/x} \tan\phi\sec\phi.d\phi$$ You can integrate it on your own.

You can proceed on simillar basis for Electric field. But before integrating you'll have to take components of field along Axis and perpendicular because it's a vector and cannot be added directly.

You'll get Field integrand as $$dE_x=\dfrac{2GM}{R^2}\times \int_0^{tan^{-1}R/x } \dfrac{tan\phi\sec\phi}{sec^2\phi} d\phi$$.

Whereas along Y you'll get no field by symmetric argument.

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