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The height \(y\) and the distance \(x\) along the horizontal plane of a projectile on a certain planet (with no surrounding atmosphere) are given by \(y=\left(8 t-5 t^{2}\right) \mathrm{m}\) and \(x=6 t \mathrm{~m}\), where \(t\) is in seconds. The velocity with which the projectile is projected at \(t=0\) is (1) \(8 \mathrm{~m} \mathrm{~s}^{-1}\) (2) \(6 \mathrm{~ms}^{-1}\) (3) \(10 \mathrm{~ms}^{-1}\) (4) Not obtainable from the data

Short Answer

Expert verified
The velocity of the projectile at launch is 10 m/s.

Step by step solution

01

Understanding the problem

The problem asks for the velocity at which the projectile is launched, given equations for its height and horizontal distance with time. The velocity vector will have both horizontal and vertical components.
02

Identify the function for velocity

The velocity of a projectile at any time is given by the first derivative of the position with respect to time. The two components are: horizontal velocity (1 dx/dt) and vertical velocity (1 dy/dt).
03

Calculate horizontal velocity component

The horizontal position is given by \(x = 6t\). Differentiating this with respect to \(t\), we get \(\frac{dx}{dt} = 6\, \text{ms}^{-1}\).
04

Calculate vertical velocity component

The vertical position is given by \(y = 8t - 5t^2\). Differentiating this with respect to \(t\), we get \(\frac{dy}{dt} = 8 - 10t\). At \(t=0\), \(\frac{dy}{dt} = 8\, \text{ms}^{-1}\).
05

Determine the launch velocity

The initial velocity of the projectile is the vector sum of its horizontal and vertical components at \(t=0\). This is calculated using the Pythagorean theorem: \(v = \sqrt{(\frac{dx}{dt})^2 + (\frac{dy}{dt})^2}\).
06

Calculate the resultant velocity

Substitute the values found: \(v = \sqrt{6^2 + 8^2} = \sqrt{36 + 64} = \sqrt{100} = 10\, \text{ms}^{-1}\). Hence, the velocity is \(10 \text{ ms}^{-1}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Velocity Calculation
In projectile motion, the velocity at which an object is launched is a crucial aspect of understanding its trajectory. Velocity is a vector quantity, meaning it has both magnitude and direction. To determine the initial velocity of a projectile, you often need to calculate its horizontal and vertical components separately and then combine them. In our scenario, the projectile's velocity at launch involves both these components. Using calculus, particularly differentiation, we find expressions for these components by deriving them from the projectile's position functions. Once the horizontal and vertical velocities are found, we use the Pythagorean theorem to calculate the magnitude of the resultant velocity. This gives us the initial speed of the projectile, helping us predict how it will move through space.
Horizontal and Vertical Components
The initial velocity of a projectile can be broken down into two crucial components: horizontal and vertical. Each plays a vital role in the object's overall motion and trajectory.
  • The horizontal component comes from the expression for horizontal position over time: \(x = 6t\). Differentiating with respect to time gives us the horizontal velocity \( \frac{dx}{dt} = 6 \, \text{ms}^{-1} \).
  • The vertical component is derived from the height equation: \(y = 8t - 5t^2\). Differentiating this, we get \( \frac{dy}{dt} = 8 - 10t\). At the initial time \(t = 0\), the vertical velocity is \(8 \, \text{ms}^{-1} \).
These components are vectors themselves, with the horizontal component representing constant speed and the vertical representing motion affected by the planet's gravity.
Differentiation in Physics
Differentiation is a fundamental mathematical technique in physics used to understand how quantities change over time. For projectile motion, differentiation helps us derive velocity from position functions, providing insight into how quickly an object’s speed and direction are changing. When given position equations for motion, taking the derivative with respect to time gives us the object's velocity. The equations \(x = 6t\) and \(y = 8t - 5t^2\) represent the position of the projectile in both horizontal and vertical dimensions. By differentiating:
  • For the horizontal position, the derivative \( \frac{dx}{dt} \) results in a constant velocity of \(6 \, \text{ms}^{-1} \), indicating no acceleration.
  • For the vertical position, the derivative \( \frac{dy}{dt} = 8 - 10t \) shows a changing velocity due to gravitational influence.
By applying differentiation, we unlock deeper understanding about the object's initial motion and its subsequent trajectory, highlighting any influences like gravitational pull overtaking the initial thrust.

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Most popular questions from this chapter

A swimmer wishes to cross a \(500-\mathrm{m}\) river flowing at \(5 \mathrm{~km} \mathrm{~h}^{-1}\). His speed with respect to water is \(3 \mathrm{~km} \mathrm{~h}^{-1}\). The shortest possible time to cross the river is (1) \(10 \mathrm{~min}\) (2) \(20 \mathrm{~min}\) (3) \(6 \mathrm{~min}\) (4) \(7.5 \mathrm{~min}\)

Ram and Shyam are walking on two perpendicular tracks with speed \(3 \mathrm{~ms}^{-1}\) and \(4 \mathrm{~m} \mathrm{~s}^{-1}\), respectively. At a certain moment (say \(\mathrm{t}=0 \mathrm{~s}\) ), Ram and Shyam are at \(20 \mathrm{~m}\) and \(40 \mathrm{~m}\) away from the intersection of tracks, respectively, and moving towards the intersection of the tracks. During the motion the magnitude of velocity of ram with respect to Shyam is (1) \(1 \mathrm{~ms}^{1}\) (2) \(4 \mathrm{~ms}^{-1}\) (3) \(5 \mathrm{~ms}^{1}\) (4) \(7 \mathrm{~ms}^{-1}\)

A shot is fired from a point at a distance of \(200 \mathrm{~m}\) from the foot of a tower \(100 \mathrm{~m}\) high so that it just passes over i horizontally. The direction of shot with horizontal is (1) \(30^{\circ}\) (2) \(45^{\circ}\) (3) \(60^{\circ}\) (4) \(70^{\circ}\)

A person initially at rest throws a ball upward with speed \(10 \mathrm{~m} / \mathrm{s}\) at angle \(37^{\circ}\) with horizontal. He tries to catch the ball. For this, he accelerates just after he throws the ball, with constant acceleration for \(1 \mathrm{sec}\) and then continues to run at a constant speed and catches the ball exactly at the same height he throws the ball. Choose the correct option(s). (Use \(\left.g=10 \mathrm{~m} / \mathrm{s}^{2}\right)\) (1) Constant speed of person is approx. \(13.7 \mathrm{~m} / \mathrm{s}\) (2) Acceleration of person is \(15.2 \mathrm{~m} / \mathrm{s}^{2}\) (3) Acceleration of person is approx. \(13.2 \mathrm{~m} / \mathrm{s}^{2}\) (4) Speed of person is \(23 \mathrm{~m} / \mathrm{s}\)

We know that when a boat travels in water, its net velocity w.r.t. ground is the vector sum of two velocities. First is the velocity of boat itself in river and other is the velocity of water w.r.t. ground. Mathematically: \(\vec{v}_{\text {boat }}=\vec{v}_{\text {boat, water }}+\vec{v}_{\text {water }}\) Now given that velocity of water w.r.t. ground in a river is \(u\). Width of the river is \(d\). A boat starting from rest aims perpendicular to the river with an acceleration of \(a=5 t\), where \(t\) is time. The boat starts from point \((1,0)\) of the coordinate system as shown in figure. Assume SI units. Find the drift of the boat when it is in the middle of the river. (1) \(u\left(\frac{3 d}{5}\right)^{1 / 3}\) (2) \(u\left(\frac{3 d}{5}\right)^{1 / 3}+1\) (3) \(u\left(\frac{6 d}{5}\right)^{1 / 3}\) (4) None of these

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