Graphing θ=π/4 on a Polar Coordinate System

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lightlightsup
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Homework Statement
Graph ##θ=\frac{π}{4}## on a Polar Coordinate System.
Relevant Equations
Why does the line go into the opposite quadrant as well?
When you graph something like ##θ=\frac{π}{4}## on a Polar Coordinate System:
Why does the line go into the opposite quadrant as well?
I can intuitively understand why it is in the first quadrant: ##θ = 45°## there and so all possible values of ##r## would apply there, giving you a straight line headed outwards at an angle of ##45°##.
So, why does the line go into the opposite quadrant as well?
Isn't ##r## always positive? Or, is that something we define beforehand as being either positive or negative?
Blank polar grid with labeled angles from 0 to 23π/12 in twelfth-π steps, concentric circles and radial lines, with a blue circle drawn around the middle ring.
Polar grid with dashed concentric circles and radial lines over Cartesian x and y axes, with a thick line through the origin along the diagonal from lower left to upper right.
 
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In polar coordinates, the angle that corresponds to a certain point is not unique. For example, let's say that we have a point, at a distance of 2 units from the origin on the radius with ##θ=30^0##. It has polar coordinates ##r=2,θ=30^0##. It has also coordinates ##r=2,θ=−330^0## and ##r=2,θ=390^0##. So, it depends on what direction we traverse the circle - as in Trigonometry an angle ##θ## is positive when it runs counter-clockwise, and how many times we traverse the circle.

EDIT: Also, the radius ##r##, can be negative. So, we talk about an oriented distance. For instance, the radius with ##θ=30^0## and the one with ##θ=210^0## form a straight line which passes through the origin. The point, say, ##P(2,210^0)## which is at a distance of ##2## units from the origin on the radius with ##θ=210^0##, has polar coordinates ##r=2,θ=210^0##. We can reach this point if we go in the positive direction ##210^0## and walk ##2## units forward. We can also reach the same point if we turn ##30^0## in the positive direction and walk ##2## units backwards. The turns we take are with reference to the initial radius (##\theta = 0##), given that we are at the origin (##O##). So, the previous point we talked about, has also polar coordinates ##r = -2, \theta = 30^0##.
 
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QuantumQuest said:
In polar coordinates, the angle that corresponds to a certain point is not unique. For example, let's say that we have a point, at a distance of 2 units from the origin on the radius with ##\theta = 30^0##. It has polar coordinates ##r = 2, \theta = 30^0##. It has also coordinates ##r = 2, \theta = -330^0## and ##r = 2, \theta = 390^0##. So, it depends on what direction we traverse the circle - as in Trigonometry an angle ##\theta## is positive when it runs counter-clockwise, and how many times we traverse the circle.
But, in my question above, isn't the opposite angle ##225°## and not some other angle equivalent to ##45°## (like ##-315°## or ##405°##)?
Am I stuck thinking in terms of the unit circle definition?
 
If you don't allow negative radius, I think you are right. Then it should be a half line in the first quadrant. Changing the angle to an equivalent doesn't change this.
 
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QuantumQuest said:
EDIT: Also, the radius rr, can be negative. So, we talk about an oriented distance. For instance, the radius with θ=300θ=30^0 and θ=2100θ=210^0 form a straight line which passes through the origin. The point P(2,2100)P(2,210^0) which is at a distance, say, of 2 units from the origin on the radius with θ=2100θ=210^0, has polar coordinates r=2,θ=2100r=2,θ=210^0. We can reach this point if we go in the positive direction 2100210^0 and walk 2 units forward. We can also reach the same point if we turn 30030^0 in the positive direction and walk 2 units backwards. The turns we take are with reference to the initial radius (θ=0\theta = 0), given that we are at the origin (OO). So, the previous point we talked about has also polar coordinates r=−2,θ=300r = -2, \theta = 30^0.
So, it's kind of like ##-\hat{r}##?
But, in the formal/mathematical case, we would explicitly have to state what ##r## is allowed to be (like ##-r##)?

So, the way I'm understanding the sign on ##θ## is that it is defined independently in each quadrant based on whether it is counterclockwise (+) or clockwise (-):
For example: ##+30°## would occur in Quadrants I and III because it would be ##30°## counterclockwise from the Polar x-Axis there. ##-30°## would occur in Quadrants II and IV because it would be clockwise from the Polar x-Axis there.
So, the mystery remains: how is ##r##'s sign defined? Left or Right from the Polar y-Axis?
Polar coordinate grid with the pole at the origin and the polar axis along the positive x-axis. Points (r, θ), (−r, θ), (r, −θ) and (−r, −θ) are plotted with dashed rays through the pole, and θ is marked as an angle from the polar axis.
 
lightlightsup said:
So, the mystery remains: how is ##r##'s sign defined?

There is no mystery. It's all a matter of convention. In math, conventions are there in order to talk about the same things in the same way. For the angle ##\theta## we use the positive sign (##+##) when we traverse the circle counter-clockwise and negative sign (##-##) when we traverse it clockwise. For the radius ##r## we use positive sign when we move from the origin to the outer side of the circle(s) on a certain radius and negative sign in the opposite case.
 
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So, the convention is that ##r## is ##+## when it is in the ##+## direction of the Polar x-Axis.
And, ##θ##'s signage is determined by clockwise/counterclockwise angling relative to the Polar x-Axis.
Does that seem like a correct interpretation?
I can't think of any other explanation for why, by convention, ##(−r,−θ)## is in Quadrant II and ##(r,−θ)## is in Quadrant IV.
Another convention I've seen is that ##r## is always pointing outwards based on how the ##θ (+ or -)## guides it. But, it can point it in the opposite direction with a ##-## before the ##r##. This is the correct answer, I think. Determine the angle first, then figure out which direction you're heading in.
Polar coordinate grid with the pole at the origin and the polar axis pointing right, showing points (r, θ), (−r, −θ), (−r, θ) and (r, −θ) connected by rays through the pole, with θ marked as an arc from the polar axis.

This is why when you graph ##θ=\frac{π}{4}##, you include it in Quadrants I and III: you are considering all values of ##r## for which ##θ=\frac{π}{4}##?
 
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lightlightsup said:
So, the convention is that ##r## is ##+## when it is in the ##+## direction of the Polar x-Axis.
And, ##θ##'s signage is determined by clockwise/counterclockwise angling relative to the Polar x-Axis.
Does that seem like a correct interpretation?
I can't think of any other explanation for why, by convention, ##(−r,−θ)## is in Quadrant II and ##(r,−θ)## is in Quadrant IV.
Another convention I've seen is that ##r## is always pointing outwards based on how the ##θ (+ or -)## guides it. But, it can point it in the opposite direction with a ##-## before the ##r##. This is the correct answer, I think. Determine the angle first, then figure out which direction you're heading in.
View attachment 255485
This is why when you graph ##θ=\frac{π}{4}##, you include it in Quadrants I and III: you are considering all values of ##r## for which ##θ=\frac{π}{4}##?

The whole point is the reference you use. In my example in post #2 I talked about the different polar coordinates of the same point. In the diagram you give, there is the same angle ##\theta## with different sign per case. So, in the first quadrant as per your diagram, we have obviously ##(r,\theta)##. In the second quadrant the angle is ##-\theta## as it is seen clockwise beginning from the negative ##-x## axis. Then, the radius is ##-r## with respect to the direction we move. In the same manner we find the signs of ##r## and ##\theta## in the rest two quadrants.
 
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Think about the equation y = 2 in a rectangular coordinate system. Why is this a line that goes both to the left and the right? Because x can be any real value and the statement is still true. It is the same for polar coordinates. If I say θ=π/4, then r can be any value, positive or negative.
 
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