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A 0.7 -lb particle is located at the position \(\mathbf{r}_{1}=\) \(2 \mathbf{i}+3 \mathbf{j}+\mathbf{k}\) ft and has the velocity \(\mathbf{v}_{1}=\mathbf{i}+\mathbf{j}+\) \(2 \mathbf{k} \mathrm{ft} / \mathrm{sec}\) at time \(t=0 .\) If the particle is acted upon by a single force which has the moment \(\mathbf{M}_{O}=(4+\) \(2 t) \mathbf{i}+\left(3-t^{2}\right) \mathbf{j}+5 \mathbf{k}\) lb-ft about the origin \(O\) of the coordinate system in use, determine the angular momentum about \(O\) of the particle when \(t=4\) sec.

Short Answer

Expert verified
The angular momentum at \( t=4 \) is approximately \( 32 \mathbf{i} + 4\mathbf{j} + 20 \mathbf{k} \text{ lb-ft-s}. \)

Step by step solution

01

Understand Angular Momentum Definition

Angular momentum, denoted by \( \mathbf{H}_O \), about the origin \( O \) for a particle is given by the cross product \( \mathbf{r} \times \mathbf{p} \), where \( \mathbf{r} \) is the position vector, and \( \mathbf{p} \) is the linear momentum (\( \mathbf{p} = m \mathbf{v} \)). The unit for angular momentum in this context is \( \text{lb-ft-s} \).
02

Calculate Linear Momentum

First, convert the weight of the particle to mass: the weight is 0.7 lb. Using \( g = 32.2 \text{ ft/s}^2 \), the mass \( m \) is \( \frac{0.7}{32.2} \approx 0.0217 \) slugs. Linear momentum \( \mathbf{p} = m \mathbf{v}_1 = 0.0217 (\mathbf{i} + \mathbf{j} + 2\mathbf{k}) \approx 0.0217\mathbf{i} + 0.0217\mathbf{j} + 0.0434\mathbf{k} \text{ lb-ft/s}. \)
03

Compute Angular Momentum at t=0

Using \( \mathbf{r}_1 = 2\mathbf{i} + 3\mathbf{j} + \mathbf{k} \), compute the cross product \( \mathbf{r}_1 \times \mathbf{p} \). The cross-product is: \[ (2\mathbf{i} + 3\mathbf{j} + \mathbf{k}) \times (0.0217\mathbf{i} + 0.0217\mathbf{j} + 0.0434\mathbf{k}) = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \ 2 & 3 & 1 \ 0.0217 & 0.0217 & 0.0434 \end{vmatrix}. \] Calculate this determinant to find \( \mathbf{H}_O(t=0). \)
04

Determine Angular Momentum at t=4 by Integrating Moment of Force

Angular momentum changes under the effect of a moment of force. Given \( \mathbf{M}_O(t) = (4 + 2t)\mathbf{i} + (3 - t^2)\mathbf{j} + 5\mathbf{k} \), we estimate change in angular momentum as \[ \Delta \mathbf{H}_O = \int_0^4 \mathbf{M}_O(t) \, dt = \int_0^4 ((4 + 2t)\mathbf{i} + (3 - t^2)\mathbf{j} + 5\mathbf{k}) \, dt. \] Compute each component: \(- \int_0^4 (4 + 2t) dt = [4t + t^2]_0^4, \) \(- \int_0^4 (3 - t^2) dt = [3t - \frac{t^3}{3}]_0^4, \) \(- \int_0^4 5 dt = [5t]_0^4. \)
05

Calculate Final Angular Momentum

Evaluate the definite integrals for each component:\[ \int_0^4 (4 + 2t) dt = [4(4) + 16] = 32, \int_0^4 (3 - t^2) dt = [12 - \frac{64}{3}] = \frac{36}{3}, \int_0^4 5 dt = 20, \]Thus, \( \Delta \mathbf{H}_O = 32\mathbf{i} + \frac{12}{3}\mathbf{j} + 20\mathbf{k}. \)Adding \( \mathbf{H}_O(t=0) \), previously found by substitution, to \( \Delta \mathbf{H}_O \), gives \( \mathbf{H}_O(t=4). \) Calculate this result.

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Key Concepts

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

Linear Momentum
Linear momentum is a fundamental concept in physics, often just called momentum. It describes the quantity of motion an object possesses and is dependent on mass and velocity. The formula for linear momentum is expressed as:
  • \( \mathbf{p} = m \mathbf{v} \)
Here, \( m \) represents the mass of the object, and \( \mathbf{v} \) stands for its velocity. This concept is particularly significant in collision and movement analyses.In our exercise, we needed to first convert the particle's weight into mass using the gravitational constant, \( g = 32.2 \text{ ft/s}^2 \), resulting in a mass of about 0.0217 slugs. This mass was then multiplied by the given velocity vector \( \mathbf{v}_1 = \mathbf{i} + \mathbf{j} + 2 \mathbf{k} \) ft/s to find the linear momentum, \( \mathbf{p} \). Breakdowns of calculations like these help illustrate how linear momentum is integral to analyzing motions.
Moment of Force
The moment of force, also known as torque, is a measure of the tendency of a force to rotate an object about a pivot point or axis. It's given by the expression:
  • \( \mathbf{M} = \mathbf{r} \times \mathbf{F} \)
In this formula, \( \mathbf{r} \) is the position vector from the axis to the point of force application, and \( \mathbf{F} \) is the force vector.In the exercise, the moment of force about the origin \( O \) was provided as a function of time \( t \):
  • \( \mathbf{M}_O(t) = (4 + 2t)\mathbf{i} + (3 - t^2)\mathbf{j} + 5\mathbf{k} \)
Understanding the moment of force is essential as it describes how forces cause rotations, directly affecting angular momentum. By integrating these forces over time, we can estimate changes in the system's angular momentum.
Cross Product
The cross product is a mathematical operation used in vector algebra to find a vector that is perpendicular to two given vectors. It's crucial in calculating physical quantities like torque and angular momentum.The cross product of two vectors \( \mathbf{A} = a_1\mathbf{i} + a_2\mathbf{j} + a_3\mathbf{k} \) and \( \mathbf{B} = b_1\mathbf{i} + b_2\mathbf{j} + b_3\mathbf{k} \) is determined by the following determinant:\[ \mathbf{A} \times \mathbf{B} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \ a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \end{vmatrix}\]This operation results in a new vector, which in physics helps understand rotational forces and moment interactions.In the context of the provided exercise, the cross product was used to compute the initial angular momentum \( \mathbf{H}_O(t=0) \) by crossing the position vector \( \mathbf{r}_1 = 2\mathbf{i} + 3\mathbf{j} + \mathbf{k} \) with the linear momentum \( \mathbf{p} \). Such applications of the cross product help unravel deeper insights into rotational dynamics.
Position Vector
A position vector is a mathematical description of the position of a point in space relative to an origin. It's one of the foundational vectors in expressing the dynamics of particles and rigid bodies.Position vectors are represented as:
  • \( \mathbf{r} = x\mathbf{i} + y\mathbf{j} + z\mathbf{k} \)
Here, \( x, y, \) and \( z \) are scalar components that specify the particle's position along the axes of a coordinate system.In our exercise, the position vector \( \mathbf{r}_1 \) was \( 2\mathbf{i} + 3\mathbf{j} + \mathbf{k} \) feet. This vector specified the particle's location at time \( t = 0 \) and was essential in calculating angular momentum through the cross-product with linear momentum.Understanding position vectors allows students to visualize and map a point's trajectory in three-dimensional space, an important skill in physics and engineering.

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Most popular questions from this chapter

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