Let A1, A2, A3, A4,........, A8 be the vertices of the regular octagons that lie on the circle of radius 2. Let p be a point on the circle and let PAi denote the distance between the point P and Ai for i = 1,2,3,....,8. If P varies over the circle, then the maximum value of the product is PA1.PA2..........PA8, is

According to the question, Ai are 8th root of 28 & let P be 2eiα.
Now, z8 – 28 = (z – A1) (z – A2) ……… (z – A8)
So, Put z = 2eiα
⇒ 28ei8α – 28 = (2eiα – A1) (2eiα – A2) (2eiα – A3) ….. (2eiα – A8)
⇒ 28 |ei8α – 1| = |(2eiα – A1) (2eiα – A2) (2eiα – A3) ….. (2eiα – A8)|
⇒ 28 |ei4α – e–i4α | = |(2eiα – A1) (2eiα – A2) (2eiα – A3) ….. (2eiα – A8)|
⇒ 29 |sin4α| = |(2eiα – A1) (2eiα – A2) (2eiα – A3) ….. (2eiα – A8)|
So, from this we get that :
Maximum value of the PA1.PA2 …… PA8 = 29
Therefore, the correct answer is 29 = 512.
The reaction sequence given below is carried out with 16 moles of X. The yield of the major product in each step is given below the product in parentheses. The amount (in grams) of S produced is ____. 
Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
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The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
In mathematics, Geometry is one of the most important topics. The concepts of Geometry are defined with respect to the planes. So, Geometry is divided into three categories based on its dimensions which are one-dimensional geometry, two-dimensional geometry, and three-dimensional geometry.
Let's consider line ‘L’ is passing through the three-dimensional plane. Now, x,y, and z are the axes of the plane, and α,β, and γ are the three angles the line making with these axes. These are called the plane's direction angles. So, correspondingly, we can very well say that cosα, cosβ, and cosγ are the direction cosines of the given line L.

Read More: Introduction to Three-Dimensional Geometry