\(\frac{\sqrt3}{\sqrt2}\)
\(\frac{\sqrt5}{\sqrt2}\)
\(\frac{\sqrt3}{\sqrt4}\)
To analyze the problem, we need to consider the equations of motion for both projectiles.
The time of flight T for a projectile launched from a height h is given by:
\( T = \frac{2v \sin(\theta)}{g} + \sqrt{\frac{2h}{g}}, \)
where v is the initial speed of projection, \(\theta\) is the angle of projection with the horizontal, g is the acceleration due to gravity, and h is the height of the launch point above the ground.
For both projectiles, the total height of the tower is \( h = 400 \, \text{m} \).
For Projectile A (\(\theta = 45^\circ\)):
\( T_A = \frac{2v_A \sin(45^\circ)}{g} + \sqrt{\frac{2 \times 400}{g}}. \)
Since \(\sin(45^\circ) = \frac{\sqrt{2}}{2}\), this becomes:
\( T_A = \frac{2v_A \cdot \frac{\sqrt{2}}{2}}{g} + \sqrt{\frac{800}{g}} = \frac{v_A \sqrt{2}}{g} + \sqrt{\frac{800}{g}}. \)
For Projectile B (\(\theta = 60^\circ\)):
\( T_B = \frac{2v_B \sin(60^\circ)}{g} + \sqrt{\frac{2 \times 400}{g}}. \)
Since \(\sin(60^\circ) = \frac{\sqrt{3}}{2}\), this becomes:
\( T_B = \frac{2v_B \cdot \frac{\sqrt{3}}{2}}{g} + \sqrt{\frac{800}{g}} = \frac{v_B \sqrt{3}}{g} + \sqrt{\frac{800}{g}}. \)
Equating the Times of Flight:
It is given that \( T_A = T_B \), so:
\( \frac{v_A \sqrt{2}}{g} + \sqrt{\frac{800}{g}} = \frac{v_B \sqrt{3}}{g} + \sqrt{\frac{800}{g}}. \)
Cancelling \(\sqrt{\frac{800}{g}}\) from both sides:
\( \frac{v_A \sqrt{2}}{g} = \frac{v_B \sqrt{3}}{g}. \)
Simplify:
\( v_A \sqrt{2} = v_B \sqrt{3}. \)
Finding the Ratio of Speeds: Rearranging for \(\frac{v_A}{v_B}\):
\( \frac{v_A}{v_B} = \frac{\sqrt{3}}{\sqrt{2}}. \)
This can be written as:
\( \frac{v_A}{v_B} = \sqrt{\frac{3}{2}}. \)
The motion of an airplane is represented by the velocity-time graph as shown below. The distance covered by the airplane in the first 30.5 seconds is km.
Due to presence of an em-wave whose electric component is given by \( E = 100 \sin(\omega t - kx) \, NC^{-1} \), a cylinder of length 200 cm holds certain amount of em-energy inside it. If another cylinder of same length but half diameter than previous one holds same amount of em-energy, the magnitude of the electric field of the corresponding em-wave should be modified as:
Let \( \alpha, \beta \) be the roots of the equation \( x^2 - ax - b = 0 \) with \( \text{Im}(\alpha) < \text{Im}(\beta) \). Let \( P_n = \alpha^n - \beta^n \). If \[ P_3 = -5\sqrt{7}, \quad P_4 = -3\sqrt{7}, \quad P_5 = 11\sqrt{7}, \quad P_6 = 45\sqrt{7}, \] then \( |\alpha^4 + \beta^4| \) is equal to:
Kinematics is a branch of physics that deals with the study of motion, without considering the forces that cause the motion. It is concerned with the position, velocity, and acceleration of objects, as well as the time it takes for them to move from one point to another.
In kinematics, the motion of an object is represented using mathematical equations and graphs. The most common quantities used in kinematics are displacement, velocity, acceleration, and time.
Displacement refers to the change in position of an object, and it is represented by the symbol Δx. Velocity is the rate at which an object's position changes over time, and it is represented by the symbol v. Acceleration is the rate at which an object's velocity changes over time, and it is represented by the symbol a.
Also Read: Kinematics Formula
By analyzing the relationships between these quantities, kinematics can be used to predict the motion of objects in different situations. For example, kinematics can be used to calculate the maximum height reached by a projectile, the distance traveled by a car during a given time, or the time it takes for a rollercoaster to complete a loop.
Kinematics is used in many areas of physics, including mechanics, astrophysics, and robotics. It is also used in engineering, where it is used to design and optimize the motion of machines and vehicles.