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A small toy airplane is flying in the \(x y\) -plane parallel to the ground. In the time interval \(t=0\) to \(t=1.00 \mathrm{s}\) its velocity as a function of time is given by \(\vec{v}=\left(1.20 \mathrm{m} / \mathrm{s}^{2}\right) t \hat{\imath}+\left[12.0 \mathrm{m} / \mathrm{s}-\left(2.00 \mathrm{m} / \mathrm{s}^{2}\right) t\right] \hat{\boldsymbol{J}}\) . At \(\quad\) what value of \(t\) is the velocity of the plane perpendicular to itsM acceleration?

Short Answer

Expert verified
The plane's velocity is perpendicular to its acceleration at \( t \approx 4.41 \) seconds.

Step by step solution

01

Understand Velocity and Acceleration

The velocity of the plane is given by \( \vec{v}(t) = (1.20t) \hat{\imath} + (12.0 - 2.00t) \hat{\boldsymbol{J}}~\mathrm{m/s} \). Acceleration is the derivative of velocity with respect to time, \( \vec{a}(t) = \frac{d\vec{v}}{dt} = (1.20) \hat{\imath} - (2.00) \hat{\boldsymbol{J}} \).
02

Calculate Acceleration

Taking the derivative of the velocity function: \( \frac{d\vec{v}}{dt} = (1.20) \hat{\imath} + (-2.00) \hat{\boldsymbol{J}} \). Hence, \( \vec{a}(t) = 1.20 \hat{\imath} - 2.00 \hat{\boldsymbol{J}} \).
03

Condition for Perpendicularity

Vectors are perpendicular if their dot product is zero. Therefore, set the dot product of \( \vec{v}(t) \) and \( \vec{a}(t) \) to zero: \( \vec{v}(t) \cdot \vec{a}(t) = 0 \).
04

Compute the Dot Product

Calculate the dot product: \( \vec{v}(t) \cdot \vec{a}(t) = (1.20t)(1.20) + (12.0 - 2.00t)(-2.00) = 0 \). Simplify to get: \( 1.44t - 24.0 + 4.00t = 0 \).
05

Solve for \( t \)

Combine like terms: \( 5.44t - 24.0 = 0 \). Solving for \( t \), \( t = \frac{24.0}{5.44} \approx 4.41 \).
06

Conclude Solution

The time \( t \) at which the velocity of the plane is perpendicular to the acceleration is approximately \( t = 4.41 \) seconds.

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Key Concepts

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

Velocity and Acceleration
Understanding velocity and acceleration is crucial in physics, especially when analyzing how objects move. Velocity is a vector quantity that describes the rate at which an object changes its position, incorporating both speed and direction.
In the exercise, the velocity of the toy airplane is given as a function of time, meaning it changes with time. The velocity \( \vec{v}(t) = (1.20t) \hat{\imath} + (12.0 - 2.00t) \hat{\boldsymbol{J}} \, \mathrm{m/s} \) specifically shows how the airplane's movement adjusts in the horizontal and vertical directions.
Acceleration, on the other hand, indicates how much the velocity changes over time. It is the derivative of the velocity function with respect to time, giving us \( \vec{a}(t) = (1.20) \hat{\imath} - (2.00) \hat{\boldsymbol{J}} \).
  • Velocity relates to the position change.
  • Acceleration details how this change in position is becoming faster or slower.
Dot Product
The dot product, also known as the scalar product, is a crucial operation in vector calculus. It takes two vectors and returns a single scalar (a number), providing important information about the vectors' orientation relative to each other.
For two vectors to be perpendicular (or orthogonal), their dot product must equal zero. In our problem, the task is to find the value of time \( t \) when the velocity vector is perpendicular to the acceleration vector, meaning their dot product is zero.
This requirement is implemented as follows: \( \vec{v}(t) \cdot \vec{a}(t) = (1.20t)(1.20) + (12.0 - 2.00t)(-2.00) = 0 \). Simplifying this expression helps us find when the vectors meet this condition.
  • Dot product yields information on the angles between vectors.
  • Perpendicular vectors have a dot product of zero.
Derivatives
Derivatives are fundamental in calculus and act as the foundation for understanding changes in quantities. They describe the rate at which one variable changes in relation to another.
In the context of this problem, the derivative of the velocity with respect to time gives us the acceleration. This allows us to understand how the velocity changes over time. Taking the derivative of \( \vec{v}(t) = (1.20t) \hat{\imath} + (12.0 - 2.00t) \hat{\boldsymbol{J}} \) results in the acceleration vector \( \vec{a}(t) = 1.20 \hat{\imath} - 2.00 \hat{\boldsymbol{J}} \. \)
  • Velocity's derivative with respect to time is acceleration.
  • Derivatives help in finding rates of change.
By differentiating, we quantify how swiftly velocity changes, which is key for dynamic systems.
Perpendicular Vectors
In vector calculus, perpendicular vectors are fundamental due to their unique properties. Vectors are perpendicular when they intersect at right angles, implying that their dot product equals zero.
This orthogonality is significant when analyzing velocity and acceleration. For our airplane, at a specific time \( t \), the velocity is perpendicular to the acceleration if their dot product is zero. This provides a simple yet powerful condition used in the solution process: \( \vec{v}(t) \cdot \vec{a}(t) = 0 \).
  • Perpendicular vectors indicate unique directional properties.
  • When examining motion, it shows non-aligning forces or motions.
Understanding when vectors are perpendicular helps in applications like force balancing and analyzing motion trajectories.

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Most popular questions from this chapter

Martian Athletics. In the long jump, an athlete launches herself at an angle above the ground and lands at the same height, trying to travel the greatest horizontal distance. Suppose that on earth she is in the air for time \(T\) , reaches a maximum height \(h,\) and achieves a horizontal distance \(D .\) If she jumped in exactly the same way during a competition on Mars, where \(g_{\text {Mars}}\) is 0.379 of its earth value, find her time in the air, maximum height, and horizontal distance. Express each of these three quantities in terms of its earth value. Air resistance can be neglected on both planets.

A shot putter releases the shot some distance above the level ground with a velocity of \(12.0 \mathrm{m} / \mathrm{s}, 51.0^{\circ}\) above the horizontal. The shot hits the ground 2.08 s later. You can ignore air resistance. (a) What are the components of the shot's acceleration while in flight? (b) What are the components of the shot's velocity at the beginning and at the end of its trajectory? (c) How far did she throw the shot horizontally? (d) Why does the expression for \(R\) in Example 3.8 not give the correct answer for part \((\mathrm{c}) ?\) (e) How high was the shot above the ground when she released it? \((\mathrm{f})\) Draw \(x-t\) , \(y-t, v_{x}-t,\) and \(v_{y}-t\) graphs for the motion.

A Ferris wheel with radius 14.0 \(\mathrm{m}\) is turning about a horizontal axis through its center (Fig. E3.29). The linear speed of a passenger on the rim is constant and equal to 7.00 \(\mathrm{m} / \mathrm{s} .\) What are the magnitude and direction of the passenger's acceleration as she passes through (a) the lowest point in her circular motion? (b) The highest point in her circular motion? (c) How much time does it take the Ferris wheel to make one revolution?

At its Ames Research Center, NASA uses its large "20-G" centrifuge to test the effects of very large accelerations ("hypergravity") on test pilots and astronauts. In this device, an arm 8.84 m long rotates about one end in a horizontal plane, and the astronaut is strapped in at the other end. Suppose that he is aligned along the arm with his head at the outermost end. The maximum sustained acceleration to which humans are subjected in this machine is typically 12.5\(g\) . (a) How fast must the astronaut's head be moving to experience this maximum acceleration? (b) What is the difference between the acceleration of his head and feet if the astronaut is 2.00 \(\mathrm{m}\) tall? (c) How fast in rpm (rev/min) is the arm turning to produce the maximum sustained acceleration?

A web page designer creates an animation in which a dot on a computer screen has a position of \(\vec{r}=[4.0 \mathrm{cm}+\) \(\left(2.5 \mathrm{cm} / \mathrm{s}^{2}\right) t^{2} ] \hat{\boldsymbol{\imath}}+(5.0 \mathrm{cm} / \mathrm{s}) t \hat{\boldsymbol{J}}\) (a) Find the magnitude and direction of the dot's average velocity between \(t=0\) and \(t=2.0 \mathrm{s} .\) (b) Find the magnitude and direction of the instantaneous velocity at \(t=0, t=1.0 \mathrm{s},\) and \(t=2.0 \mathrm{s} .\) (c) Sketch the dot's trajectory from \(t=0\) to \(t=2.0 \mathrm{s},\) and show the velocities calculated in part (b).

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