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An object is tracked by a radar station and determined to have a position vector given by \(\vec{r}=(3500-160 t) \hat{\mathrm{i}}+2700 \hat{\mathrm{j}}+300 \hat{\mathrm{k}}\), with \(\vec{r}\) in meters and \(t\) in seconds. The radar station's \(x\) axis points east. its \(y\) axis north, and its \(z\) axis vertically up. If the object is a \(250 \mathrm{~kg}\) meteorological missile, what are (a) its linear momentum, (b) its direction of motion, and (c) the net force on it?

Short Answer

Expert verified
(a) Linear momentum: \(-40000 \hat{\mathrm{i}}\) kg·m/s. (b) Direction: westward. (c) Net force: 0 N.

Step by step solution

01

Understanding Linear Momentum

The linear momentum \( \vec{p} \) of an object is given by the product of its mass \( m \) and its velocity \( \vec{v} \). First, we compute the velocity by differentiating the position vector \( \vec{r} \) with respect to time \( t \). The velocity \( \vec{v} \) is: \( \vec{v} = \frac{d\vec{r}}{dt} = (-160) \hat{\mathrm{i}} \). Now, with mass \( m = 250 \mathrm{~kg} \), the linear momentum is \( \vec{p} = m \cdot \vec{v} = 250 \times (-160) \hat{\mathrm{i}} \). Therefore, \( \vec{p} = -40000 \hat{\mathrm{i}} \) kg·m/s.
02

Determining Direction of Motion

The direction of motion is determined by the velocity vector \( \vec{v} \). Since the velocity vector \( \vec{v} = -160 \hat{\mathrm{i}} \), the direction of motion is along the negative \( x \)-axis, which points westward.
03

Calculating Net Force

The net force \( \vec{F} \) can be determined using Newton's second law \( \vec{F} = m \cdot \vec{a} \), where \( \vec{a} \) is the acceleration. Since the velocity \( \vec{v} = -160 \hat{\mathrm{i}} \) is constant (does not depend on \( t \)), the acceleration \( \vec{a} = \frac{d\vec{v}}{dt} = 0 \). Therefore, the net force \( \vec{F} = 250 \times 0 = 0 \).

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Key Concepts

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

Velocity Vector
The concept of a velocity vector is essential to understanding motion in a three-dimensional space. A velocity vector describes the speed and direction of an object. It is derived from the position vector by calculating its time derivative. In the given problem, the position vector is \( \vec{r}=(3500-160 t) \hat{\mathrm{i}}+2700 \hat{\mathrm{j}}+300 \hat{\mathrm{k}} \), and so, to find the velocity vector \( \vec{v} \), we differentiate with respect to time \( t \). This gives us \( \vec{v} = \frac{d\vec{r}}{dt} = (-160) \hat{\mathrm{i}} \). The vector indicates:
  • a speed of 160 meters per second.
  • a direction along the negative \( x \)-axis, meaning toward the west.
This singular direction and speed signify uniform or constant motion along a straight path without any deviation into the \( y \) or \( z \) axes.
Direction of Motion
Direction of motion is straightforward when you have a clear velocity vector. Here, the velocity vector \( \vec{v} = -160 \hat{\mathrm{i}} \) exemplifies this concept by pointing towards a defined direction. Since the velocity has a negative component only in the \( \hat{\mathrm{i}} \) direction, the motion is purely westward in alignment with the negative \( x \)-axis. This makes it convenient to understand where the object is heading:
  • If an axis is positive, moving in the negative direction means opposite to that sense.
  • The absence of components in \( \hat{\mathrm{j}} \) or \( \hat{\mathrm{k}} \) shows no movements north or vertically up, respectively.
Thus, an understanding of vectors straight away tells you all about the directional movement of objects in a physics problem.
Net Force
In physics, net force propels an object, but understanding how it plays with constant velocity helps solve problems like this. Newton's second law \( \vec{F} = m \cdot \vec{a} \) relates force, mass, and acceleration. Here, the velocity is constant, \( \vec{v} = -160 \hat{\mathrm{i}} \), indicating no change in speed or direction. Therefore, acceleration \( \vec{a} \) is zero. With zero acceleration:
  • The net force \( \vec{F} = 250 \times 0 = 0 \) Newtons.
  • This indicates a state of equilibrium where all external forces, if any, balance out, resulting in steadiness in motion.
Knowing there's no net force helps understand that steady motion signifies balance without additional push or pull.
Acceleration
Acceleration tells us about the changes in velocity. A non-zero acceleration implies changes in speed, direction, or both. In our problem, we already know the velocity \( \vec{v} \) is constant (-160 meters per second in the \( \hat{\mathrm{i}} \) direction). To find acceleration, you need to differentiate velocity with time:
  • If \( \vec{v} \) is constant: \( \vec{a} = \frac{d\vec{v}}{dt} = 0 \).
The zero acceleration means:
  • The object maintains a steady speed.
  • The direction of travel does not alter.
An understanding of acceleration in such problems clarifies that an object in such a state continues moving uniformly without any unexpected changes.

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Most popular questions from this chapter

An electron undergoes a one-dimensional elastic collision with an initially stationary hydrogen atom. What percentage of the electron's initial kinetic energy is transferred to kinetic energy of the hydrogen atom? (The mass of the hydrogen atom is 1840 times the mass of the electron.)

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Figure 9-44 shows an arrangement with an air track, in which a cart is connected by a cord to a hanging block. The cart has mass \(m_{1}=0.600 \mathrm{~kg}\), and its center is initially at \(x y\) coordinates \((-0.500\) \(\mathrm{m}, 0 \mathrm{~m}) ;\) the block has mass \(m_{2}=0.400 \mathrm{~kg}\), and its center is initially at \(x y\) coordinates \((0,-0.100 \mathrm{~m})\). The mass of the cord and pulley are negligible. The cart is released from rest, and both cart and block move until the cart hits the pulley. The friction between the cart and the air track and between the pulley and its axle is negligible. (a) In unit-vector notation, what is the acceleration of the center of mass of the cart-block system? (b) What is the velocity of the com as a function of time \(t ?\) (c) Sketch the path taken by the com. (d) If the path is curved, determine whether it bulges upward to the right or downward to the left, and if it is straight, find the angle between it and the \(x\) axis.

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