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AA moving circle with variable size has plane parallel to the  
\[yz\]
  plane, passes through the line  
\[y=0, \; z=a\]
  and has a chord in common with the circle  
\[x^2+y^2=a^2, \; z=0\]
, As the circle moves it generates a volume.
To meet the conditions at  
\[x=0\]
  the circle must have radius  
\[a\]
  and centre  
\[(0,0)\]
  and to meet the conditions at  
\[x= \pm a\]
  it must have radius  
\[r= \frac{a}{2}\]
  and centre at  
\[z= \frac{a}{2}\]
  so the circle must obey an equation of the form  
\[y^2+(z-p)^2=r^2\]
  where  
\[p, \; r\]
  are both functions of  
\[x\]
.
For the stationary circle  
\[(x_1,y_1)\]
  satisfy  
\[y_1= \sqrt{a^2-x^2_1}\]
  and this is equal to half a chord.  
\[(x_1,y_1)\]
  is also a point on the moving circle with  
\[z=0\]
  so we can write  
\[y^2_1+p^2=r^2\]
.
The moving circle passes through  
\[y=0, \; z=a\]
  so  
\[a^2-2ap+[^2=r^2\]
.
Solving these two equations simultaneously, we have  
\[y^2_1=a^2-2ap\]
  from which  
\[p=\frac{a^2y^1_1}{2a}= \frac{a^2-(a^2-x^2_1)}{2a}=\frac{x^2_1}{2a}\]
  then  
\[r^2=y^2_1+p^2=a^2-x^2_1+ \frac{x^4_1}{4a^2}\]
.
A disc of radius  
\[r\]
  and thickness  
\[\Delta x\]
  at  
\[x_1\]
  has volume  
\[\Delta V = \pi r^2 \Delta x = \pi (a^2-x^2_1+ \frac{x^4_1}{4a^2}) \Delta x \]
  and the total volume traced by the moving circle is  
\[V = \pi \int^a_{-a} (a^2-x^2_1+ \frac{x^4_1}{4a^2}) dx =\frac{43 \pi a^3}{30}\]
.