Chapter 12: Problem 42
Calculate the work done in the following situations. A constant force \(\mathbf{F}=\langle 2,4,1\rangle\) (in newtons) moves an object from (0,0,0) to \((2,4,6) .\) (Distance is measured in meters.)
Short Answer
Expert verified
Answer: The work done in moving the object is 26 Joules.
Step by step solution
01
Calculate the displacement vector
The displacement vector is the difference between the final position and the initial position of the object. We are given the coordinates of the initial position as (0,0,0) and the final position as (2,4,6). Thus, the displacement vector can be computed as:
\(\mathbf{d}=\langle 2-0,4-0,6-0\rangle=\langle 2,4,6\rangle\)
02
Find the dot product of the force and displacement vectors
To calculate the work done, we need to find the dot product of the force vector \(\mathbf{F}\) and the displacement vector \(\mathbf{d}\). The dot product is given by:
\(\mathbf{F} \cdot \mathbf{d} = F_x \cdot d_x + F_y \cdot d_y + F_z \cdot d_z\)
where \(F_x,F_y,\) and \(F_z\) represent the x, y, and z components of the force vector, and \(d_x,d_y,\) and \(d_z\) represent the x, y, and z components of the displacement vector.
Now substituting the given values we get:
\(\mathbf{F} \cdot \mathbf{d} = (2)(2) + (4)(4) + (1)(6) = 4 + 16 + 6 = 26\)
03
Calculate the work done
Finally, the work done is equal to the dot product of the force vector and the displacement vector. Thus, the work done in moving the object from the initial position to the final position is:
Work Done = \(\mathbf{F} \cdot \mathbf{d} = 26 \text{ Joules}\)
Unlock Step-by-Step Solutions & Ace Your Exams!
-
Full Textbook Solutions
Get detailed explanations and key concepts
-
Unlimited Al creation
Al flashcards, explanations, exams and more...
-
Ads-free access
To over 500 millions flashcards
-
Money-back guarantee
We refund you if you fail your exam.
Over 30 million students worldwide already upgrade their learning with Vaia!
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Displacement Vector
When an object moves from one position to another, we describe this movement using a displacement vector. This vector is particularly important because it captures the change in position in terms of direction and magnitude.
In our example, the object moves from the initial position
\[\mathbf{d} = \langle 2-0, 4-0, 6-0 \rangle = \langle 2,4,6 \rangle\]
This vector
In our example, the object moves from the initial position
- (0,0,0)
- (2,4,6)
\[\mathbf{d} = \langle 2-0, 4-0, 6-0 \rangle = \langle 2,4,6 \rangle\]
This vector
- Represents the direction in which the object moved
- Illustrates the distance it covered in the x, y, and z directions
Dot Product
The dot product is a key operation when working with vectors, especially in physics. It is used to determine quantities like work, where both direction and magnitude matter. The dot product of two vectors essentially projects one vector onto another and multiplies by the magnitude.
For our case, we calculate the dot product of the force vector
\[\mathbf{F} \cdot \mathbf{d} = F_x \cdot d_x + F_y \cdot d_y + F_z \cdot d_z\]
Breaking it down into components, we multiply the corresponding x, y, and z components:
\[(2)(2) + (4)(4) + (1)(6) = 4 + 16 + 6 = 26\]
Through the dot product, we calculate how much of the force is effectively being used in moving the object along the direction of displacement. This scalar result represents the work done.
For our case, we calculate the dot product of the force vector
- \(\mathbf{F} = \langle 2,4,1 \rangle\)
- \(\mathbf{d} = \langle 2,4,6 \rangle\)
\[\mathbf{F} \cdot \mathbf{d} = F_x \cdot d_x + F_y \cdot d_y + F_z \cdot d_z\]
Breaking it down into components, we multiply the corresponding x, y, and z components:
- \(F_x = 2\), \(d_x = 2\)
- \(F_y = 4\), \(d_y = 4\)
- \(F_z = 1\), \(d_z = 6\)
\[(2)(2) + (4)(4) + (1)(6) = 4 + 16 + 6 = 26\]
Through the dot product, we calculate how much of the force is effectively being used in moving the object along the direction of displacement. This scalar result represents the work done.
Vector Components
Vectors are physical quantities that have both magnitude and direction, and they are often broken down into components to simplify calculations. The components of a vector are essentially the projections of the vector onto the x, y, and z axes.
For a vector \(\mathbf{v} = \langle v_x, v_y, v_z \rangle\), each component represents how much of the vector's magnitude is aligned with each coordinate axis.
In our scenario, the force vector \(\mathbf{F}\) and the displacement vector \(\mathbf{d}\) both have three components:
For a vector \(\mathbf{v} = \langle v_x, v_y, v_z \rangle\), each component represents how much of the vector's magnitude is aligned with each coordinate axis.
In our scenario, the force vector \(\mathbf{F}\) and the displacement vector \(\mathbf{d}\) both have three components:
- Force vector: \(\mathbf{F} = \langle 2, 4, 1 \rangle\)
- Displacement vector: \(\mathbf{d} = \langle 2, 4, 6 \rangle\)
- We preserve the directionality of the vectors
- The calculations become manageable and more intuitive