
We start by applying the law of sines to the sides and angles of the triangle:
\(\frac{a + d}{\sin A} = \frac{a}{\sin B} = \frac{a - d}{\sin C} = 2\)
From this, we deduce that \( A = \frac{\pi}{2} + C \).
Using the identity for sine, we have:
\(\sin A = \sin \left( \frac{\pi}{2} + C \right) = \cos C\)
Now, using the relationship between the sides:
\(\frac{a + d}{2} = \sqrt{1 - \sin^2 C}\)
\(\Rightarrow \left( \frac{a + d}{2} \right)^2 = 1 - \left( \frac{a - d}{2} \right)^2\)
Expanding and simplifying, we get:
\(2(a^2 + d^2) / 4 = 1 \quad \Rightarrow \quad a^2 + d^2 = 2\)
From this, we get Equation (1):
\(a^2 + d^2 = 2\)
Next, we use the cosine law to relate angle \( B \):
\(\cos B = \frac{(a - d)^2 + (a + d)^2 - a^2}{2(a^2 - d^2)}\)
Simplifying further, we get:
\(\sqrt{1 - \sin^2 B} = \frac{2(a^2 + d^2) - a^2}{2(a^2 - d^2)} \quad \Rightarrow \quad a^2 = \frac{7}{4}, \, d^2 = \frac{1}{4}\)
Now, we can find the area \( \Delta \) of the triangle using the formula:
\(\Delta = \frac{a(a^2 - d^2)}{4}\)
Substitute the values of \( a^2 \) and \( d^2 \):
\(\alpha = \frac{\sqrt{7}}{2} \times \frac{6}{4 \times 4}\)
Finally, we find that:
\((64 \alpha)^2 = 1008\)
Thus, the value of \( (64 \alpha)^2 \) is 1008.
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
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