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A \(2.0 \mathrm{~kg}\) particle-like object moves in a plane with velocity components \(v_{x}=30 \mathrm{~m} / \mathrm{s}\) and \(v_{y}=60 \mathrm{~m} / \mathrm{s}\) as it passes through the point with \((x, y)\) coordinates of \((3.0,-4.0) \mathrm{m}\). Just then, in unitvector notation, what is its angular momentum relative to (a) the origin and (b) the point located at \((-2.0,-2.0) \mathrm{m} ?\)

Short Answer

Expert verified
(a) 600 kg m²/s, (b) 720 kg m²/s

Step by step solution

01

Understanding Angular Momentum

Angular momentum for a particle can be calculated using the formula: \( \mathbf{L} = \mathbf{r} \times \mathbf{p} \) where \( \mathbf{r} \) is the position vector, \( \mathbf{p} \) is the linear momentum given by \( \mathbf{p} = m \mathbf{v} \), and \( m \) is the mass of the object. The cross product signifies the perpendicular effect of the velocity on the position vector.
02

Calculate Velocity's Linear Momentum

The linear momentum \( \mathbf{p} \) is found from \( \mathbf{p} = m \times \mathbf{v} \). Given, \( m = 2.0 \) kg, \( v_x = 30 \) m/s, and \( v_y = 60 \) m/s. Calculate: \[ \mathbf{p} = 2.0 \times (30 \hat{i} + 60 \hat{j}) = 60 \hat{i} + 120 \hat{j} \text{ kg m/s} \]
03

Determine Position Vector for Part A

For part (a), the position from the origin is given by the vector from the origin to the point (3.0, -4.0) m. Thus, \( \mathbf{r}_{\text{origin}} = 3.0 \hat{i} - 4.0 \hat{j} \) m.
04

Calculate Angular Momentum for Part A

Use the formula \( \mathbf{L} = \mathbf{r} \times \mathbf{p} \). Perform the cross product:\[ \mathbf{L}_{\text{origin}} = (3 \hat{i} - 4 \hat{j}) \times (60 \hat{i} + 120 \hat{j}) \]This results in:\[ \mathbf{L}_{\text{origin}} = (3 \times 120 - (-4) \times 60) \hat{k} = (360 + 240) \hat{k} = 600 \hat{k} \text{ kg m}^2/\text{s} \]
05

Determine Position Vector for Part B

For part (b), calculate position from the point (-2.0, -2.0) to (3.0, -4.0). The position vector becomes \( \mathbf{r}_{(-2, -2)} = (3 - (-2)) \hat{i} + (-4 - (-2)) \hat{j} = 5 \hat{i} - 2 \hat{j} \) m.
06

Calculate Angular Momentum for Part B

Use \( \mathbf{L} = \mathbf{r} \times \mathbf{p} \) with the new \( \mathbf{r} \):\[ \mathbf{L}_{(-2, -2)} = (5 \hat{i} - 2 \hat{j}) \times (60 \hat{i} + 120 \hat{j}) \]Calculate the cross product:\[ \mathbf{L}_{(-2, -2)} = (5 \times 120 - (-2) \times 60) \hat{k} = (600 + 120) \hat{k} = 720 \hat{k} \text{ kg m}^2/\text{s} \]
07

Conclusion

The angular momentum of the object is different depending on the reference point. It is \( 600 \hat{k} \) kg m²/s relative to the origin and \( 720 \hat{k} \) kg m²/s relative to the point (-2.0, -2.0).

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Key Concepts

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

Cross Product
The cross product is a fundamental concept in vector mathematics, particularly in three dimensions. It is used to calculate the angular momentum of an object, among other things. The cross product of two vectors \( \mathbf{A} \) and \( \mathbf{B} \) is denoted by \( \mathbf{A} \times \mathbf{B} \) and results in a vector that is perpendicular to the plane formed by the two original vectors.
The magnitude of the cross product is calculated as: \[ \| \mathbf{A} \times \mathbf{B} \| = \| \mathbf{A} \| \| \mathbf{B} \| \sin(\theta) \] where \( \theta \) is the angle between \( \mathbf{A} \) and \( \mathbf{B} \). The direction of the resulting vector is determined by the right-hand rule.
  • The cross product is crucial in physics because it describes rotational effects.
  • In calculating angular momentum \( \mathbf{L} = \mathbf{r} \times \mathbf{p} \), it combines linear momentum \( \mathbf{p} \) and position vector \( \mathbf{r} \).
The perpendicular nature of the cross product makes it particularly useful for describing rotations, such as when determining how an object will spin around a particular axis or point.
Linear Momentum
Linear momentum is a measure of an object's motion. It is a vector quantity and depends on two things: the object's mass and its velocity. It is given by the formula:\[ \mathbf{p} = m \mathbf{v} \]where \( m \) is the mass and \( \mathbf{v} \) is the velocity of the object.
Linear momentum has the same direction as the velocity vector because mass is a scalar quantity, it only scales the velocity vector without changing its direction.
  • For our problem, we have a particle of mass \( 2.0 \text{ kg} \).
  • The velocity components are \( v_x = 30 \text{ m/s} \) and \( v_y = 60 \text{ m/s} \).
  • Thus the linear momentum is \( \mathbf{p} = 60 \hat{i} + 120 \hat{j} \text{ kg m/s}\).
In any closed system, the total linear momentum is conserved, which means that the sum of momenta before an interaction equals the sum after. This principle is fundamental in collision and explosion analyses.
Position Vector
The position vector describes a point in space relative to a reference origin. It is a core component in calculating angular momentum using the formula \( \mathbf{L} = \mathbf{r} \times \mathbf{p} \). The position vector \( \mathbf{r} \) plays a crucial role by determining the line along which the object moves and the pivot point for rotational calculations.
  • For part (a) of the exercise, the position vector from the origin to the point \((3.0, -4.0) \text{ m}\) is \(3.0 \hat{i} - 4.0 \hat{j} \text{ m}\).
  • In part (b), from point \((-2.0, -2.0) \text{ m}\) to \((3.0, -4.0) \text{ m}\), it is \(5 \hat{i} - 2 \hat{j} \text{ m}\).
Choosing the right position vector is essential in rotational dynamics. It can change the magnitude and direction of angular momentum, as demonstrated by differing outcomes when altering the reference point.
Mass and Velocity
Mass and velocity are key factors in determining the linear momentum of an object. Together, they dictate both the speed and the inertial resistance of a moving object.
  • Mass \( m \) is a measure of the quantity of matter in an object, expressed in kilograms.
  • Velocity \( \mathbf{v} \) has both magnitude and direction, expressed in meters per second (m/s).
In the context of momentum, mass provides a measure of how much force is needed to change an object's motion. If mass is constant, as in most simple physics problems, velocity changes directly influence momentum.
  • In our exercise, the mass is \(2.0 \text{ kg}\) and the velocity is given by components: \(v_x = 30 \text{ m/s}\) and \(v_y = 60 \text{ m/s}\).
  • This translates into a velocity vector \( \mathbf{v} = 30 \hat{i} + 60 \hat{j} \text{ m/s}\).
Both factors, combined together, shape an object's linear momentum and therefore contribute heavily towards the calculation of its angular momentum through the cross product with the position vector.

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Most popular questions from this chapter

An automobile traveling at \(80.0 \mathrm{~km} / \mathrm{h}\) has tires of \(75.0 \mathrm{~cm}\) diameter. (a) What is the angular speed of the tires about their axles? (b) If the car is brought to a stop uniformly in \(30.0\) complete turns of the tires (without skidding), what is the magnitude of the angular acceleration of the wheels? (c) How far does the car move during the braking?

A body of radius \(R\) and mass \(m\) is rolling smoothly with speed \(v\) on a horizontal surface. It then rolls up a hill to a maximum height \(h\). (a) If \(h=3 v^{2} / 4 g\), what is the body's rotational inertia about the rotational axis through its center of mass? (b) What might the body be?

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In 1980 , over San Francisco Bay, a large yo-yo was released from a crane. The \(116 \mathrm{~kg}\) yo-yo consisted of two uniform disks of radius \(32 \mathrm{~cm}\) connected by an axle of radius \(3.2 \mathrm{~cm} .\) What was the magnitude of the acceleration of the yo-yo during (a) its fall and (b) its rise? (c) What was the tension in the cord on which it rolled? (d) Was that tension near the cord's limit of \(52 \mathrm{kN}\) ? Suppose you build a scaled-up version of the yo-yo (same shape and materials but larger). (e) Will the magnitude of your yo-yo's acceleration as it falls be greater than, less than, or the same as that of the San Francisco yo-yo? (f) How about the tension in the cord?

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