/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 3 A body is projected with velocit... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A body is projected with velocity \(u\) at an angle of projection \(\theta\) with the horizontal. The direction of velocity of the body makes angle \(30^{\circ}\) with the horizontal at \(t=2 \mathrm{~s}\) and then after \(1 \mathrm{~s}\) it reaches the maximum height. Then (1) \(u=20 \sqrt{3} \mathrm{~m} \mathrm{~s}^{-1}\) (2) \(\theta=60^{\circ}\) (3) \(\theta=30^{\circ}\) (4) \(u=10 \sqrt{3} \mathrm{~ms}^{-1}\)

Short Answer

Expert verified
The correct options are (1) and (2).

Step by step solution

01

Express velocity in terms of components

The initial velocity of the body is given as \(u\), which can be broken into horizontal and vertical components. The horizontal component is \(u \cos \theta\) and the vertical component is \(u \sin \theta\).
02

Use the velocity direction relation at \(t=2\) s

At \(t=2\) seconds, the angle between the velocity and the horizontal is \(30^{\circ}\). Therefore, \(\tan 30^{\circ} = \frac{v_y}{v_x}\) where \(v_x = u \cos \theta\) and \(v_y = u \sin \theta - g \cdot 2\). Hence, solve: \[ \frac{u \sin \theta - g \cdot 2}{u \cos \theta} = \frac{1}{\sqrt{3}} \]
03

Equation for reaching maximum height after 1 second

The object reaches maximum height 1 second after \(t=2\) seconds, so at \(t=3\) seconds. At maximum height, the vertical component of velocity becomes zero: \[ u \sin \theta - g \cdot 3 = 0 \] This simplifies to \(u \sin \theta = 30 \).
04

Solve equations to find \(u\) and \(\theta\)

We have two equations from Steps 2 and 3:1. \(u \sin \theta = 30\)2. \(\frac{30 - 20}{u \cos \theta} = \frac{1}{\sqrt{3}}\)Solve for \(u \cos \theta\) from equation 2: \(u \cos \theta = 10 \sqrt{3}\).Use these results:- \(\tan \theta = \frac{30}{10\sqrt{3}} = \sqrt{3}\), so \(\theta = 60^{\circ}\).- \(u = \frac{30}{\sin 60^{\circ}} = 20 \sqrt{3} \; \text{m/s}\).
05

Select the correct answer

From the calculations, \(u=20 \sqrt{3} \; \text{m/s}\) and \(\theta=60^{\circ}\). Therefore, the correct options are (1) and (2).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Initial Velocity Components
When a projectile is launched, understanding its initial velocity components is crucial. The initial velocity, denoted as \(u\), can be split into two parts, describing its motion in both the horizontal and vertical directions.
In mathematical terms, the horizontal component of velocity is \(u \cos \theta\). This component describes how quickly the projectile moves along the horizontal plane. The vertical component is \(u \sin \theta\) and represents the speed at which the projectile ascends or descends.
These components are essential because they help us to understand and predict the overall motion of the projectile. For instance, they allow us to calculate how high or how far the projectile will travel and determine its behavior at different times during its flight.
Angle of Projection
The angle of projection, \(\theta\), plays a vital role in shaping the projectile's path. It is the angle at which a projectile is launched concerning the horizontal plane. This angle influences both how high and how far the projectile will travel.
A larger angle tends to result in a higher trajectory, allowing the projectile to reach greater heights. Conversely, a smaller angle will produce a flatter trajectory, which may cover more horizontal distance if the initial velocity is constant.
In this particular exercise, the angle of projection is \(60^{\circ}\), as calculated from the equations. Understanding this angle is key to determining the time it takes to reach certain points, such as when the projectile reaches maximum height or when it returns to the ground.
Maximum Height
The maximum height of a projectile is the peak point of its trajectory. At this point, the vertical component of its velocity (\(v_y\)) becomes zero. The projectile momentarily stops moving upward and starts descending.
In our exercise, we calculated that the projectile reaches this maximum height at \(t = 3\) seconds. This was determined by the equation \(u \sin \theta - g \cdot 3 = 0\), which signifies that the vertical velocity component decreases due to gravity until it reaches zero.
Knowing the maximum height is important because it helps us understand the duration of the projectile's ascent and can be used to calculate its potential energy at that highest point.
Horizontal and Vertical Components of Velocity
The horizontal and vertical components of velocity determine the shape and length of a projectile's path. These components change over time due to gravity's influence.
The horizontal component, \(v_x = u \cos \theta\), remains constant throughout the projectile's motion because there are no horizontal forces acting under ideal conditions without air resistance.
In contrast, the vertical component, \(v_y = u \sin \theta - g \cdot t\), decreases over time as gravity pulls the projectile downward. At its peak, as noted, \(v_y = 0\), after which it becomes negative as the projectile descends.
Understanding these components allows us to predict the projectile's landing point and how long it stays in the air. They are fundamental in solving problems involving projectile motion, like the one in our exercise, where we use them to find the angle and initial speed.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A river is flowing towards with a velocity of \(5 \mathrm{~m} \mathrm{~s}^{-1}\). The boat velocity is \(10 \mathrm{~m} \mathrm{~s}^{-1}\). The boat crosses the river by shortest path. Hence, (1) The direction of boat's velocity is \(30^{\circ}\) west of north. (2) The direction of boat's velocity is north-west. (3) Resultant velocity is \(5 \sqrt{3} \mathrm{~m} \mathrm{~s}^{-1}\). (4) Resultant velocity of boat is \(5 \sqrt{2} \mathrm{~m} \mathrm{~s}^{-1}\).

A particle is projected with a certain velocity at an angle \(\alpha\) above the horizontal from the foot of an inclined plane of inclination \(30^{\circ}\). If the particle strikes the plane normally. then \(\alpha\) is equal to (1) \(30^{\circ}+\tan ^{-1}\left(\frac{\sqrt{3}}{2}\right)\) (2) \(45^{\circ}\) (3) \(60^{\circ}\) (4) \(30^{\circ}+\tan ^{-1}(2 \sqrt{3})\)

A body is thrown with the velocity \(v_{0}\) at an angle of \(\theta\) to the horizon. Determine \(v_{0}\) in \(\mathrm{ms}^{-1}\) if the maximum height attained by the body is \(5 \mathrm{~m}\) and at the highest point of its trajectory the radius of curvature is \(r=3 \mathrm{~m}\). Neglect air resistance. [Use \(\sqrt{80}\) as 9 ]

Projectile motion is a combination of twe enslonal motions: one in horizontal and other in vertical direction. Motion in \(2 D\) means in a plane. Necessary condition for \(2 D\) motion is that the velocity vector is coplanar to the acceleration vector. In case of projectile motion, the angle between velocity and acceleration will be \(0^{\circ}<\theta<180^{\circ} .\) During the projectile motion, the horizontal component of velocity remains unchanged but vertical component of velocity is time dependent. Now answer the following questions: A body is projected at angle of \(30^{\circ}\) and \(60^{\circ}\) with ?e same velocity. Their horizontal ranges are \(R_{1}\) and \(R\), nd maximum heights are \(H_{1}\) and \(H_{2}\), respectively, then (1) \(\frac{R_{1}}{R_{2}}>1\) (2) \(\frac{H_{1}}{H_{2}}>1\) (3) \(\frac{R_{\mathrm{I}}}{R_{2}}<1\) (4) \(\frac{H_{1}}{H_{2}}<1\)

A projectile has initially the same horizontal velocin as it would acquire if it had moved from rest with unifon acceleration of \(3 \mathrm{~m} \mathrm{~s}^{-2}\) for \(0.5 \mathrm{~min}\). If the maximum heigis reached by it is \(80 \mathrm{~m}\), then the angle of projection ip \(\left(g=10 \mathrm{~ms}^{-2}\right)\) (1) \(\tan ^{-1} 3\) (2) \(\tan ^{-1}(3 / 2)\) (3) \(\tan ^{-1}(4 / 9)\) (4) \(\sin ^{-1}(4 / 9)\)

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.