A stone is thrown horizontally from the top of a 20 m high building with a speed of 12 m/s. It hits the ground at a distance R from the building. Taking g = 10 m/s2 and neglecting air resistance will give :
This problem involves analyzing the motion of a stone thrown horizontally from a height, which is a classic example of projectile motion. In projectile motion, we typically analyze the horizontal and vertical components of motion independently, assuming air resistance is negligible.
We are given:
We need to find the horizontal distance \(R\) the stone travels before hitting the ground.
The stone is thrown horizontally, which means its initial vertical velocity is zero (\(v_{yi} = 0\)). The vertical motion is governed by gravity, causing a constant downward acceleration (\(a_y = g = 10\) m/s\(^2\)). The stone falls a vertical distance equal to the height of the building, \(h = 20\) m.
We can use the following kinematic equation for vertical displacement:
\(\Delta y = v_{yi}t + \frac{1}{2}a_yt^2\)
Let's take the downward direction as positive. So, initial vertical velocity \(v_{yi} = 0\), vertical displacement \(\Delta y = h = 20\) m, and acceleration \(a_y = g = 10\) m/s\(^2\). Let \(t\) be the time taken to hit the ground.
\(20 = (0)t + \frac{1}{2}(10)t^2\)
\(20 = 5t^2\)
\(t^2 = \frac{20}{5}\)
\(t^2 = 4\)
Taking the square root, we get \(t = \pm 2\). Since time must be positive, the time taken for the stone to hit the ground is \(t = 2\) seconds.
Since air resistance is neglected, there is no horizontal acceleration (\(a_x = 0\)). The horizontal velocity remains constant throughout the motion. The initial horizontal speed is \(v_x = 12\) m/s.
The horizontal distance covered (the range \(R\)) is given by the product of the constant horizontal velocity and the time of flight (\(t\)):
\(R = v_x \times t\)
Using the values we found:
\(R = 12 \text{ m/s} \times 2 \text{ s}\)
\(R = 24 \text{ m}\)
The horizontal distance \(R\) from the building where the stone hits the ground is 24 m.
Comparing this result with the given options:
Our calculated value \(R = 24\) m matches Option 3.
| Aspect | Horizontal Component | Vertical Component |
|---|---|---|
| Acceleration (neglecting air resistance) | \(a_x = 0\) | \(a_y = g\) (downward) |
| Velocity | Constant (\(v_x = v_{xi}\)) | Changes due to gravity (\(v_y = v_{yi} + gt\)) |
| Displacement | \(x = v_{xi}t\) | \(y = v_{yi}t + \frac{1}{2}gt^2\) |
| Initial Velocity (Horizontal Throw) | \(v_{xi} = v_{throw}\) | \(v_{yi} = 0\) |
Understanding projectile motion is key to solving many physics problems. Here are some extra points:
A sphere of volume V is made of a material with lower density than water. While on Earth, it floats on water with its volume f1V (f1 < 1) submerged. On the other hand, on a spaceship accelerating with acceleration a < g (g is the acceleration due to gravity on Earth) in outer space, its submerged volume in water is f2V. Then:
A railway wagon (open at the top) of mass M1 is moving with speed v1 along a straight track. As a result of rain, after some time it gets partially filled with water so that the mass of the wagon becomes M2 and speed becomes v2. Taking the rain to be falling vertically and the water stationery inside the wagon, the relation between the two speeds v1 and v2 is :
Consider the following statements:
1. Distance between the longitudes becomes zero on North Pole and South Pole.
2. Distance between the longitudes is maximum on the Equator.
3. Number of longitudes is more than number of latitudes.
Which of the statements given above is/are correct?
One block of 2⋅0 kg mass is placed on top of another block of 3⋅0 kg mass. The coefficient of static friction between the two blocks is 0⋅2. The bottom block is pulled with a horizontal force F such that both the blocks move together without slipping. Taking acceleration due to gravity as 10 m/s2, the maximum value of the frictional force is :
A mass is attached to a spring that hangs vertically. The extension produced in the spring is 6 cm on Earth. The acceleration due to gravity on the surface of the Moon is one-sixth of its value on the surface of the Earth. The extension of the spring on the Moon would be: