Problem 21
Question
The graph of an equation in \(x, y\), and \(z\) is symmetric with respect to the \(x y\)-plane if replacing \(z\) by \(-z\) results in an equivalent equation. What condition leads to a graph that is symmetric with respect to each of the following? (a) \(y z\)-plane (b) \(z\)-axis (c) origin
Step-by-Step Solution
Verified Answer
(a) Replace \(x\) with \(-x\), (b) Replace \(x\) and \(y\) with \(-x\) and \(-y\), (c) Replace \(x\), \(y\), \(z\) by \(-x\), \(-y\), \(-z\).
1Step 1: Understanding Symmetry in the y-z Plane
To check for symmetry with respect to the \(y z\)-plane, we need to see if replacing \(x\) with \(-x\) gives us an equivalent equation. This occurs because each point \((x, y, z)\) reflected over the \(y z\)-plane becomes \((-x, y, z)\). Thus, the condition required is that the equation remains unchanged when \(x\) is replaced with \(-x\).
2Step 2: Understanding Symmetry in the z-axis
An equation is symmetric with respect to the \(z\)-axis if replacing both \(x\) with \(-x\) and \(y\) with \(-y\) results in an equivalent equation. This is because reflecting a point \((x, y, z)\) about the \(z\)-axis gives us \((-x, -y, z)\). Therefore, the condition for this symmetry is that the equation remains unchanged under the transformation \((x, y)\) to \((-x, -y)\).
3Step 3: Understanding Symmetry in the Origin
For a graph to be symmetric with respect to the origin, replacing \(x\) with \(-x\), \(y\) with \(-y\), and \(z\) with \(-z\) must produce an equivalent equation. This stems from the fact that reflecting any point \((x, y, z)\) through the origin results in the point \((-x, -y, -z)\). Hence, the required condition is that the equation is unchanged when all three variables are replaced by their negatives.
Key Concepts
xy-plane symmetryyz-plane symmetryz-axis symmetryorigin symmetry
xy-plane symmetry
The concept of symmetry in the context of the xy-plane is an intriguing one. Symmetry here implies, essentially, a kind of mirror reflection, which results when you replace the variable \(z\) with \(-z\) in an equation. Consider this akin to looking into a mirror that's lying flat through the xy-plane. If the equation remains unchanged after this transformation, its graph is symmetric with respect to the xy-plane. This means all points with coordinates \((x, y, z)\) have corresponding points \((x, y, -z)\), highlighting their symmetric relationship.
- This condition is common in many physical and mathematical systems, often reflecting real-world scenarios where the system experiences uniform conditions above and below a particular plane.
- Examples of such symmetry can be seen in even functions of \(z\) that consist solely of even powers, like \(z^2\) or constant terms independent of \(z\).
yz-plane symmetry
To determine symmetry with respect to the yz-plane, focus on what occurs when you replace \(x\) with \(-x\) in the equation. This is like taking each point plotted in three-dimensional space and reflecting it across the yz-plane, creating a mirror image on either side of this plane.
- If the equation remains identical after this swap, it suggests a symmetric property across the yz-plane.
- This symmetry implies that for every point \((x, y, z)\), there is an equal counterpart at \((-x, y, z)\).
z-axis symmetry
For z-axis symmetry, the process involves changing both \(x\) to \(-x\) and \(y\) to \(-y\). This results in symmetry around the z-axis, akin to spinning an object around a central vertical line and seeing no change in its appearance.
- Confirmed when every equation remains the same even after substituting both variables \(x\) and \(y\) with their negative counterparts.
- This symmetry results in each point \((x, y, z)\) having a reflected point \((-x, -y, z)\), preserving the same distance and position relative to the z-axis.
origin symmetry
Origin symmetry in three-dimensional equations entails a complete negation of all three variables: \(x\), \(y\), and \(z\). Replace them with their negatives, and check if the equation remains consistent.
- This transformation is equivalent to turning an object around, comparing it to its inverted self through the center of its coordinate system.
- An equation maintaining its form under such conditions means that every point \((x, y, z)\) correlates with \((-x, -y, -z)\).
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