/*! 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 50 A bird flies in the \(x y\) -pla... [FREE SOLUTION] | 91Ó°ÊÓ

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A bird flies in the \(x y\) -plane with a velocity vector given by \(\overrightarrow{\boldsymbol{v}}=\left(\alpha-\beta t^{2}\right) \hat{\imath}+\gamma t \hat{\jmath},\) with \(\alpha=2.4 \mathrm{~m} / \mathrm{s}, \beta=1.6 \mathrm{~m} / \mathrm{s}^{3},\) and \(\gamma=4.0 \mathrm{~m} / \mathrm{s}^{2} .\) The positive \(y\) -direction is vertically upward. At \(t=0\) the bird is at the origin. (a) Calculate the position and acceleration vectors of the bird as functions of time. (b) What is the bird's altitude (y-coordinate) as it flies over \(x=0\) for the first time after \(t=0 ?\)

Short Answer

Expert verified
The position vector of bird is \(\(\overrightarrow{\boldsymbol{r}} = (\alpha t - \frac{\beta t^{3}}{3})\hat{\imath} + \frac{\gamma t^{2}}{2}\hat{\jmath}\) and acceleration vector is -3.2t\, \hat{\imath} + 4\, \hat{\jmath}. The bird's altitude is 2.676 \, m when it flies over \(x=0\) for the first time after \(t=0\).

Step by step solution

01

Integrate the velocity vector to get position

The position vector can be obtained by integrating the velocity vector with respect to time. The velocity vector is given as\(\overrightarrow{\boldsymbol{v}}=\left(\alpha-\beta t^{2}\right)\hat{\imath}+\gamma t \hat{\jmath}\). Thus:\(\overrightarrow{\boldsymbol{r}} = \int \overrightarrow{\boldsymbol{v}}\, dt = \int (\alpha-\beta t^{2}) dt\, \hat{\imath} + \int \gamma t\, dt \, \hat{\jmath},\) where \(\alpha=2.4 \mathrm{~m} / \mathrm{s}, \beta=1.6 \mathrm{~m} / \mathrm{s}^{3}, and \(\gamma=4.0 \mathrm{~m} / \mathrm{s}^{2}\)
02

Calculate the position vector

On integrating the above expressions, the position vector becomes:\(\overrightarrow{\boldsymbol{r}} = (\alpha t - \frac{\beta t^{3}}{3})\hat{\imath} + \frac{\gamma t^{2}}{2}\hat{\jmath}\)
03

Differentiate the velocity vector to get acceleration

The acceleration vector can be obtained by differentiating the velocity vector with respect to time. It is given as:\(\overrightarrow{\boldsymbol{a}} = \frac{d\overrightarrow{\boldsymbol{v}}}{dt} = \frac{d}{dt}((\alpha - \beta t^{2})\hat{\imath} + \gamma t\hat{\jmath} = -2\beta t\, \hat{\imath} + \gamma\, \hat{\jmath}\)
04

Calculate the acceleration vector

Substituting \(\beta\) and \(\gamma\) in the above expression and simplifying, we get:\(\overrightarrow{\boldsymbol{a}} = -3.2t\, \hat{\imath} + 4\, \hat{\jmath} \mathrm{m/s}^{2}\)
05

Calculate the time when x=0 for the first time after t=0

For the bird to be flying back over x=0 after t=0 for the first time, you need to set the x-component of the position vector equal to zero and solve for time. The x-component is \(\alpha t - \frac{\beta t^{3}}{3} = 0\). Therefore, we solve the equation \(2.4t-0.53t^{3}=0\) to get \(t = 1.633 \, s\)
06

Finding the altitude when x=0 for the first time

Now, substituting \(t = 1.633 \, s\) into the y-component of the position vector, we can find bird's altitude. The y-component is \(\frac{\gamma t^{2}}{2}\), on substituting \(t\) and \( \gamma\) in the equation, we get \(y = 2(\frac{(1.633)^2}{2}) = 2.676 \, m\)

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Key Concepts

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

Vectors
Vectors are essential in physics as they not only give us magnitude but also direction. In this exercise, the bird's motion is described using a velocity vector, \(\overrightarrow{\boldsymbol{v}} = \left(\alpha - \beta t^{2}\right) \hat{\imath} + \gamma t \hat{\jmath} \), which indicates how the bird's speed and direction change over time.
The components
  • \(\alpha\), \(\beta\), and \(\gamma\) represent constants that influence the velocity.
  • The \(\hat{\imath}\) direction (usually the x-axis) signifies horizontal movement.
  • The \(\hat{\jmath}\) direction (usually the y-axis) corresponds to vertical movement.
Understanding these components helps us predict where the bird will be at any given time by examining both x and y directions.
Velocity and acceleration
Velocity indicates speed with direction. The vector changes over time as functions of \(t\) in this exercise. To understand the bird's movement, we delved into the velocity vector:
The expression \(\overrightarrow{\boldsymbol{v}} = \left(\alpha - \beta t^{2}\right) \hat{\imath} + \gamma t \hat{\jmath}\) provides insight into how the horizontal and vertical speeds vary:
  • The x-direction speed decreases over time since \(- \beta t^{2}\) becomes more significant.
  • The y-direction speed simply increases steadily due to \(\gamma t\).
Acceleration, the derivative of velocity, explores how this speed changes per time unit. By differentiating, we find the acceleration vector: \(\overrightarrow{\boldsymbol{a}} = -2\beta t \hat{\imath} + \gamma \hat{\jmath}\). Notice that horizontal acceleration depends on time \(t\), while vertical acceleration is a constant \(\gamma\).
Integration and differentiation
Integration and differentiation are powerful calculus tools used to solve motion problems like this.

Integration helps us find the position from velocity. Given the velocity vector, integration was applied to obtain the position: \(\overrightarrow{\boldsymbol{r}} = \int \overrightarrow{\boldsymbol{v}} \, dt = (\alpha t - \frac{\beta t^{3}}{3}) \hat{\imath} + \frac{\gamma t^{2}}{2} \hat{\jmath}\). This indicates the bird's exact location over time:
  • The horizontal position decreases after a certain point due to the negative \(\beta t^{3}\) term becoming dominant.
  • The vertical position increases over time as the square of \(t\).
Differentiation, on the other hand, is about understanding change rates. By differentiating the velocity, we understand how acceleration, \(-2\beta t \hat{\imath} + \gamma \hat{\jmath}\), charts the changes in speed, offering crucial insights for predicting motion dynamics.

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Most popular questions from this chapter

An object is projected with initial speed \(v_{0}\) from the edge of the roof of a building that has height \(H .\) The initial velocity of the object makes an angle \(\alpha_{0}\) with the horizontal. Neglect air resistance. (a) If \(\alpha_{0}\) is \(90^{\circ}\), so that the object is thrown straight up (but misses the roof on the way down), what is the speed \(v\) of the object just before it strikes the ground? (b) If \(\alpha_{0}=-90^{\circ}\), so that the object is thrown straight down, what is its speed just before it strikes the ground? (c) Derive an expression for the speed \(v\) of the object just before it strikes the ground for general \(\alpha_{0}\). (d) The final speed \(v\) equals \(v_{1}\) when \(\alpha_{0}\) equals \(\alpha_{1}\). If \(\alpha_{0}\) is increased, does \(v\) increase, decrease, or stay the same?

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You are a member of a geological team in Central Africa. Your team comes upon a wide river that is flowing east. You must determine the width of the river and the current speed (the speed of the water relative to the earth). You have a small boat with an outboard motor. By measuring the time it takes to cross a pond where the water isn't flowing, you have calibrated the throttle settings to the speed of the boat in still water. You set the throttle so that the speed of the boat relative to the river is a constant \(6.00 \mathrm{~m} / \mathrm{s}\). Traveling due north across the river, you reach the opposite bank in \(20.1 \mathrm{~s}\). For the return trip, you change the throttle setting so that the speed of the boat relative to the water is \(9.00 \mathrm{~m} / \mathrm{s}\). You travel due south from one bank to the other and cross the river in \(11.2 \mathrm{~s}\). (a) How wide is the river, and what is the current speed? (b) With the throttle set so that the speed of the boat relative to the water is \(6.00 \mathrm{~m} / \mathrm{s},\) what is the shortest time in which you could cross the river, and where on the far bank would you land?

A jet plane is flying at a constant altitude. At time \(t_{1}=0,\) it has components of velocity \(v_{x}=90 \mathrm{~m} / \mathrm{s}, v_{y}=110 \mathrm{~m} / \mathrm{s} .\) At time \(t_{2}=30.0 \mathrm{~s}\) the components are \(v_{x}=-170 \mathrm{~m} / \mathrm{s}, v_{y}=40 \mathrm{~m} / \mathrm{s}\). (a) Sketch the velocity vectors at \(t_{1}\) and \(t_{2} .\) How do these two vectors differ? For this time interval calculate (b) the components of the average acceleration, and (c) the magnitude and direction of the average acceleration.

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