Chapter 9: Problem 12
Graph the polar equations. $$r=1-\sin \theta$$
Short Answer
Expert verified
The graph of \( r = 1 - \sin \theta \) is a cardioid with symmetry about the vertical axis.
Step by step solution
01
Understand the Polar Equation
The given polar equation is \( r = 1 - \sin \theta \). In polar coordinates, \( r \) represents the distance from the origin, and \( \theta \) is the angle from the positive x-axis. This type of equation can represent curves like circles, limaçons, and cardioids.
02
Identify the Type of Curve
The form of the equation \( r = 1 - \sin \theta \) suggests it belongs to the family of limaçon curves. When an equation is in the form \( r = a - b\sin \theta \), and if \( a = b \), the curve is typically a cardioid.
03
Analyze the Equation for Key Features
Considering \( r = 1 - \sin \theta \), we find that both \( a \) and \( b \) equal 1. This confirms the curve is a cardioid. The maximum value of \( r \) occurs when \( \sin \theta = -1 \), giving \( r = 1 - (-1) = 2 \). The minimum value of \( r \) occurs when \( \sin \theta = 1 \), giving \( r = 1 - 1 = 0 \).
04
Plot Key Points and Symmetry
Plot points for some key angles: For \( \theta = 0\), \( r = 1 \). For \( \theta = \frac{\pi}{2} \), \( r = 0 \). For \( \theta = \pi \), \( r = 1 \). For \( \theta = \frac{3\pi}{2} \), \( r = 2 \). These points help outline the shape. The equation's symmetry about the vertical axis (since it involves \( -\sin \theta \)) indicates it will look the same on both sides.
05
Sketch the Curve
Begin plotting the graph by marking the origin at \( r = 0 \) for \( \theta = \frac{\pi}{2} \), then move around to extend to \( r = 2 \) at \( \theta = \frac{3\pi}{2} \). Complete the curve by connecting these points smoothly back to \( r = 1 \) at both \( \theta = 0 \) and \( \theta = \pi \). The shape should resemble a heart-like cardioid.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Polar Equations
Polar equations are a way to describe curves using polar coordinates, which involve a radius and an angle. Unlike the traditional Cartesian system, where points are plotted using x and y coordinates, in polar coordinates each point is indicated by
For the equation \( r = 1 - \sin \theta \), the value of \( r \) changes as \( \theta \) varies, forming a shape in the polar plane. By understanding how \( \theta \) affects \( r \), you can visualize what shape the equation will generate, such as circles or more complex curves like limaçons and cardioids.
- the distance from the origin, named \( r \), and
- the angle \( \theta \), measured from the positive x-axis.
For the equation \( r = 1 - \sin \theta \), the value of \( r \) changes as \( \theta \) varies, forming a shape in the polar plane. By understanding how \( \theta \) affects \( r \), you can visualize what shape the equation will generate, such as circles or more complex curves like limaçons and cardioids.
Cardioid
A cardioid is a special type of limaçon, and it shows up as a heart-like shape when plotted. It is a member of the limaçon family of curves, characterized by their distinctive loops and cusps. A cardioid specifically occurs when the parameters of a limaçon equation are equal, such as\( a = b \).
In the equation \( r = 1 - \sin \theta \), because 1 is both \( a \) and \( b \), it forms a cardioid.
The cardioid curve exhibits certain interesting features:
In the equation \( r = 1 - \sin \theta \), because 1 is both \( a \) and \( b \), it forms a cardioid.
The cardioid curve exhibits certain interesting features:
- Its maximum distance from the origin is twice the constant parameter (\( 2 \times 1 = 2 \)).
- The cardioid has one cusp, where the curve meets itself, typically at \( \theta = \pi \over 2 \) for this equation, resulting in \( r = 0 \).
- This shape reflects about the vertical axis due to the \(-\sin \theta \) term, showing symmetry.
Limaçon Curves
Limaçon curves form a broad category of curves in polar equations. These curves are described by equations like \( r = a - b\sin \theta \) or \( r = a - b\cos \theta \). They are fascinating due to their variety:
- If \( a = b \), you get a cardioid, a specific limaçon type.
- When \( a > b \), the limaçon appears as an outer ring or loop, sometimes called a "convex limaçon."
- If \( a < b \), the curve develops an inner loop, becoming an "inner-loop limaçon."