Problem 86
Question
Later in our study of physics we will encounter quantities represented by (\(\overrightarrow{A}\) \\(\times\\) \(\overrightarrow{B}\)) \(\cdot\) \(\overrightarrow{C}\). (a) Prove that for any three vectors \(\overrightarrow{A}\), \(\overrightarrow{B}\), and \(\overrightarrow{C}\), \(\overrightarrow{A}\) \(\cdot\) (\(\overrightarrow{B}\) \\(\times\\) \(\overrightarrow{C}\)) = (\(\overrightarrow{A}\) \\(\times\\) \(\overrightarrow{B}\)) \(\cdot\) \(\overrightarrow{C}\). (b) Calculate (\(\overrightarrow{A}\) \\(\times\\) \(\overrightarrow{B}\)) \(\cdot\) \(\overrightarrow{C}\) for vector \(\overrightarrow{A}\) with magnitude \(A\) = 5.00 and angle \(\theta$$_A\) = 26.0\(^{\circ}\) (measured from the +\(x\)-axis toward the \(+$$y\)-axis), vector \(\overrightarrow{B}\) with \(B\) = 4.00 and \(\theta$$_B\) = 63.0\(^{\circ}\), and vector \(\overrightarrow{C}\) with magnitude 6.00 and in the \(+$$z\)-direction. Vectors \(\overrightarrow{A}\) and \(\overrightarrow{B}\) are in the \(x$$y\)-plane.
Step-by-Step Solution
VerifiedKey Concepts
Vector Cross Product
The cross product of two vectors \( \overrightarrow{A} \) and \( \overrightarrow{B} \), denoted as \( \overrightarrow{A} \times \overrightarrow{B} \), can be calculated by determining the determinant of a 3x3 matrix formed by:
- The unit vectors \( \hat{i}, \hat{j}, \hat{k} \) along the \( x, y, z \) axes in the first row,
- The components of \( \overrightarrow{A} \) in the second row,
- And the components of \( \overrightarrow{B} \) in the third row.
Dot Product
For two vectors \( \overrightarrow{A} \) and \( \overrightarrow{B} \), the dot product is calculated as:\[\overrightarrow{A} \cdot \overrightarrow{B} = A_xB_x + A_yB_y + A_zB_z\]When you perform a dot product, the result is a scalar (not a vector) which essentially measures how much one vector 'projects' onto another.
A practical physical interpretation of the dot product is the calculation of work done when a force is applied at an angle to the direction of movement. Furthermore, the dot product depends on the angle \( \theta \) between the vectors, as given by:\[\overrightarrow{A} \cdot \overrightarrow{B} = |\overrightarrow{A}| |\overrightarrow{B}| \cos(\theta)\]This implies that the dot product will be zero if two vectors are orthogonal to each other since \( \cos(90°) = 0 \). In many real-world applications, this property helps in identifying whether two vectors are perpendicular.
Vector Components
Taking a vector \( \overrightarrow{A} \) as an example, it can be described by its components \((A_x, A_y, A_z)\) in a three-dimensional space. Each component represents the projection along the respective axis.
- In two-dimensional space, use trigonometry to analyse a vector's orientation: \( A_x = A \cos(\theta) \) and \( A_y = A \sin(\theta) \).
- In three-dimensional space, the vector \( \overrightarrow{A} = (A_x, A_y, A_z) \) might include components that point in the \( x, y, \) and \( z \) directions.