Chapter 11: Problem 32
What are the \(x, y,\) and \(z\) components of the angular momentum of a particle located at \(\overrightarrow{\mathbf{r}}=x \hat{\mathbf{i}}+y \hat{\mathbf{j}}+z \hat{\mathbf{k}}\) which has momentum \(\overrightarrow{\mathbf{p}}=p_{x} \hat{\mathbf{i}}+p_{y} \hat{\mathbf{j}}+p_{z} \hat{\mathbf{k}}\) ?
Short Answer
Expert verified
\(L_x = y p_z - z p_y\) ; \(L_y = z p_x - x p_z\) ; \(L_z = x p_y - y p_x\)
Step by step solution
01
Identify the cross product formula
Angular momentum \( \overrightarrow{L} \) can be calculated using the cross product of position vector \( \overrightarrow{r} = x \hat{\mathbf{i}} + y \hat{\mathbf{j}} + z \hat{\mathbf{k}} \) and momentum vector \( \overrightarrow{p} = p_x \hat{\mathbf{i}} + p_y \hat{\mathbf{j}} + p_z \hat{\mathbf{k}} \). The formula is \( \overrightarrow{L} = \overrightarrow{r} \times \overrightarrow{p} \).
02
Compute the x-component of angular momentum
Using the determinant method for computing cross products, the x-component \( L_x \) is given by eliminating the first row and first column of the determinant, resulting in:\[L_x = (y \cdot p_z - z \cdot p_y)\]
03
Compute the y-component of angular momentum
The y-component \( L_y \) is obtained by eliminating the first row and second column of the determinant, resulting in:\[L_y = (z \cdot p_x - x \cdot p_z)\]
04
Compute the z-component of angular momentum
The z-component \( L_z \) is found by eliminating the first row and third column of the determinant, which gives:\[L_z = (x \cdot p_y - y \cdot p_x)\]
05
Compile the full angular momentum vector
The resulting angular momentum vector \( \overrightarrow{L} \) is:\[\overrightarrow{L} = (y \cdot p_z - z \cdot p_y) \hat{\mathbf{i}} + (z \cdot p_x - x \cdot p_z) \hat{\mathbf{j}} + (x \cdot p_y - y \cdot p_x) \hat{\mathbf{k}}\]
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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 mathematical operation used to find a vector that is perpendicular to two given vectors. In three-dimensional space, the cross product of vectors \( \overrightarrow{a} \) and \( \overrightarrow{b} \) is denoted as \( \overrightarrow{a} \times \overrightarrow{b} \).
This operation is essential in calculating quantities like torque and angular momentum.
In the context of angular momentum, given a position vector \( \overrightarrow{r} \) and a momentum vector \( \overrightarrow{p} \), the angular momentum \( \overrightarrow{L} \) can be determined using the cross product. The direction of the resulting angular momentum vector \( \overrightarrow{L} \) will be perpendicular to both \( \overrightarrow{r} \) and \( \overrightarrow{p} \).
The formula for the cross product in vector components is as follows:
This operation is essential in calculating quantities like torque and angular momentum.
In the context of angular momentum, given a position vector \( \overrightarrow{r} \) and a momentum vector \( \overrightarrow{p} \), the angular momentum \( \overrightarrow{L} \) can be determined using the cross product. The direction of the resulting angular momentum vector \( \overrightarrow{L} \) will be perpendicular to both \( \overrightarrow{r} \) and \( \overrightarrow{p} \).
The formula for the cross product in vector components is as follows:
- \( \overrightarrow{L} = \overrightarrow{r} \times \overrightarrow{p} \)
Determinant Method
The determinant method is a systematic way to calculate the cross product of two vectors.
This method uses a 3x3 matrix to organize the unit vectors and the components of the vectors involved.
For the position vector \( \overrightarrow{r} = x \hat{\mathbf{i}} + y \hat{\mathbf{j}} + z \hat{\mathbf{k}} \) and momentum vector \( \overrightarrow{p} = p_x \hat{\mathbf{i}} + p_y \hat{\mathbf{j}} + p_z \hat{\mathbf{k}} \), the determinant form is set up as follows:
\[\begin{vmatrix} \hat{\mathbf{i}} & \hat{\mathbf{j}} & \hat{\mathbf{k}} \x & y & z \p_x & p_y & p_z\end{vmatrix}\]
This matrix is expanded to calculate each component of the resulting cross product. The structure involves:
This method uses a 3x3 matrix to organize the unit vectors and the components of the vectors involved.
For the position vector \( \overrightarrow{r} = x \hat{\mathbf{i}} + y \hat{\mathbf{j}} + z \hat{\mathbf{k}} \) and momentum vector \( \overrightarrow{p} = p_x \hat{\mathbf{i}} + p_y \hat{\mathbf{j}} + p_z \hat{\mathbf{k}} \), the determinant form is set up as follows:
\[\begin{vmatrix} \hat{\mathbf{i}} & \hat{\mathbf{j}} & \hat{\mathbf{k}} \x & y & z \p_x & p_y & p_z\end{vmatrix}\]
This matrix is expanded to calculate each component of the resulting cross product. The structure involves:
- Ignoring one of the unit vector columns while calculating the minor determinant for each.
- The first column omitted results in the \( x \)-component;
- The second column omitted gives the \( y \)-component;
- The third results in the \( z \)-component.
Momentum Vector
A momentum vector represents the motion of a particle in terms of its mass and velocity.
Defined as \( \overrightarrow{p} = p_x \hat{\mathbf{i}} + p_y \hat{\mathbf{j}} + p_z \hat{\mathbf{k}} \), it indicates how much motion a particle has and in which direction.
The components of the momentum vector \( (p_x, p_y, p_z) \) signify:
This interaction through the cross product ultimately describes the rotation or angular motion of a particle in space.
Defined as \( \overrightarrow{p} = p_x \hat{\mathbf{i}} + p_y \hat{\mathbf{j}} + p_z \hat{\mathbf{k}} \), it indicates how much motion a particle has and in which direction.
The components of the momentum vector \( (p_x, p_y, p_z) \) signify:
- \( p_x \): motion across the x-axis
- \( p_y \): motion across the y-axis
- \( p_z \): motion across the z-axis
This interaction through the cross product ultimately describes the rotation or angular motion of a particle in space.
Position Vector
The position vector is essential in determining the location of a particle in three-dimensional space.
It is expressed as \( \overrightarrow{r} = x \hat{\mathbf{i}} + y \hat{\mathbf{j}} + z \hat{\mathbf{k}} \), where \( x \), \( y \), and \( z \) describe the particle's coordinates.
Each component represents a specific axis:
The interaction between the position vector and the momentum vector through the cross product determines the complete angular momentum vector of a particle.
It is expressed as \( \overrightarrow{r} = x \hat{\mathbf{i}} + y \hat{\mathbf{j}} + z \hat{\mathbf{k}} \), where \( x \), \( y \), and \( z \) describe the particle's coordinates.
Each component represents a specific axis:
- \( x \): horizontal position along the x-axis
- \( y \): vertical position along the y-axis
- \( z \): depth position along the z-axis
The interaction between the position vector and the momentum vector through the cross product determines the complete angular momentum vector of a particle.