/*! 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 78 In the overhead view of Fig. 4-4... [FREE SOLUTION] | 91Ó°ÊÓ

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In the overhead view of Fig. 4-47, Jeeps \(P\) and \(B\) race along straight lines, across flat terrain, and past stationary border guard \(A .\) Relative to the guard, \(B\) travels at a constant speed of \(20.0 \mathrm{~m} / \mathrm{s},\) at the angle \(\theta_{2}=30.0^{\circ} .\) Relative to the guard, \(P\) has accelerated from rest at a constant rate of \(0.400 \mathrm{~m} / \mathrm{s}^{2}\) at the angle \(\theta_{1}=60.0^{\circ} .\) At a certain time during the acceleration, \(P\) has a speed of \(40.0 \mathrm{~m} / \mathrm{s}\). At that time, what are the (a) magnitude and (b) direction of the velocity of \(P\) relative to \(B\) and the (c) magnitude and (d) direction of the acceleration of \(P\) relative to \(B ?\)

Short Answer

Expert verified
(a) 24.82 m/s, (b) 83.79° above x-axis, (c) 0.400 m/s², (d) 60.0° to x-axis.

Step by step solution

01

Determine the time for Jeep P to reach the given speed

Jeep P accelerates from rest with a constant acceleration of \(0.400\,m/s^2\) until it reaches a speed of \(40.0\,m/s\). Using the equation \(v = at\), we can calculate the time \(t\): \[t = \frac{v}{a} = \frac{40.0\,m/s}{0.400\,m/s^2} = 100\,s\]
02

Calculate velocity components of Jeep P

Using the given angle \(\theta_1 = 60.0^\circ\), the velocity components of jeep P can be calculated as: \[v_{Px} = 40.0\,m/s \cdot \cos(60.0^\circ) = 20.0\,m/s\]\[v_{Py} = 40.0\,m/s \cdot \sin(60.0^\circ) = 34.64\,m/s\]
03

Calculate velocity components of Jeep B

Jeep B moves at a constant speed of \(20.0\,m/s\) and the angle \(\theta_2 = 30.0^\circ\). The velocity components for jeep B are:\[v_{Bx} = 20.0\,m/s \cdot \cos(30.0^\circ) = 17.32\,m/s\]\[v_{By} = 20.0\,m/s \cdot \sin(30.0^\circ) = 10.0\,m/s\]
04

Calculate the velocity of P relative to B

The velocity of P relative to B (\(\vec{v_{P/B}}\)) is the vector difference \(\vec{v_P} - \vec{v_B}\). Therefore, the components are:\[v_{P/Bx} = v_{Px} - v_{Bx} = 20.0\,m/s - 17.32\,m/s = 2.68\,m/s\]\[v_{P/By} = v_{Py} - v_{By} = 34.64\,m/s - 10.0\,m/s = 24.64\,m/s\]The magnitude of \(\vec{v_{P/B}}\) is:\[|\vec{v_{P/B}}| = \sqrt{(2.68)^2 + (24.64)^2} = 24.82\,m/s\]
05

Determine the direction of P's velocity relative to B

The angle of the velocity of P relative to B can be calculated using the tangent function:\[\tan\phi = \frac{v_{P/By}}{v_{P/Bx}} = \frac{24.64}{2.68}\]\[\phi = \tan^{-1}\left(\frac{24.64}{2.68}\right) = 83.79^\circ\]Therefore, the direction is \(83.79^\circ\) above the x-axis.
06

Calculate the acceleration of P relative to B

Since Jeep B does not accelerate, its acceleration is zero. The acceleration of P relative to B is the same as the acceleration of P relative to A: \[a_{P/B} = 0.400\,m/s^2\]The components are: \[a_{P/Bx} = a_{P} \cdot \cos(60.0^\circ) = 0.400\,m/s^2 \cdot 0.5 = 0.200\,m/s^2\]\[a_{P/By} = a_{P} \cdot \sin(60.0^\circ) = 0.400\,m/s^2 \cdot (\sqrt{3}/2) = 0.346\,m/s^2\]
07

Determine the direction of P's acceleration relative to B

For the relative acceleration direction, use the tangent function:\[\tan\phi = \frac{a_{P/By}}{a_{P/Bx}} = \frac{0.346}{0.200}\]\[\phi = \tan^{-1}\left(\frac{0.346}{0.200}\right) = 60.0^\circ\]Thus the direction is \(60.0^\circ\) relative to the x-axis.

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Key Concepts

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

Motion in Two Dimensions
When an object moves through space, its motion can occur in one, two, or even three dimensions. Understanding motion in two dimensions is crucial since it involves movement along both the x (horizontal) and y (vertical) axes. In our exercise, Jeeps P and B each move in a two-dimensional plane, making two-dimensional analysis necessary.

In two dimensions, the motion is determined by separate calculations for each component - x and y. This decomposition allows us to handle more complex movements by individually analyzing straightforward linear motions. The equations of motion for each axis are similar to one-dimensional motion but need to be combined to fully understand the two-dimensional path.

The use of trigonometric functions helps in resolving vectors into their components, given the angles at which objects move. This forms the backbone of analyzing relative velocity as seen in the problem.
Velocity Components
Breaking down velocity into components is essential when dealing with two-dimensional problems. The velocity of each jeep can be separated into horizontal (x) and vertical (y) components using trigonometry.

For instance, for Jeep P, the velocity components are derived from its angle of trajectory (60 degrees) and its speed (40 m/s). Therefore:
  • Horizontal velocity ( \(v_{Px}\) ): 40 m/s \(\times\) cos(60°)
  • Vertical velocity ( \(v_{Py}\) ): 40 m/s \(\times\) sin(60°)

Similarly, steps are taken for Jeep B, incorporating its constant speed (20 m/s) and angle (30 degrees).

Understanding these components allows us to simplify the interactions between two objects, as it isolates effects along each axis. This separation makes it easier to apply vector addition to identify relative motion.
Relative Acceleration
Relative acceleration focuses on how one object's acceleration appears from the perspective of another moving object. In this exercise, Jeep P is accelerating while Jeep B travels at a constant speed, leading us to consider the acceleration of P relative to B.

Since B doesn't accelerate, its contribution to the relative acceleration is zero. Thus, the relative acceleration is purely dictated by P's acceleration. The component breakdown would yield:
  • Horizontal acceleration ( \(a_{P/Bx}\) ): 0.4 m/s² \(\times\) cos(60°)
  • Vertical acceleration ( \(a_{P/By}\) ): 0.4 m/s² \(\times\) sin(60°)

Examining these components gives a complete picture of how P is accelerating from B's perspective, helping in determining direction alongside magnitude.
Vector Addition
Vector addition is a fundamental concept for solving problems involving relative velocity and acceleration. It involves adding vectors (which have both magnitude and direction) according to their components. In our exercise, the relative velocity between Jeeps is found using vector subtraction, a form of vector addition.

Consider the vectors \(\vec{v_P}\) and \(\vec{v_B}\) representing velocities of Jeeps P and B respectively. The relative velocity is given by:
  • Subtracting Jeep B's velocity components from Jeep P's components
  • Using Pythagorean theorem to find the magnitude: \(\sqrt{(v_{P/Bx})^2 + (v_{P/By})^2}\)
  • Applying tangent function to find the direction from the components

Vector addition not only aids in these calculations but also provides a visual method of interpreting motion when graphing vectors within the plane.

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