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Mathematics 21 Online
OpenStudy (anonymous):

polar graph restriction

OpenStudy (anonymous):

for the graph \[r=\frac{2}{3\sin(\theta)-\cos(\theta)} \] find the restricttions on \[\theta\] and explain what this means in terms of the graph

OpenStudy (anonymous):

We can't have the denominator equal to zero, so 3sin(theta) cannot equal cos(theta). Therefore if we divide by cos theta on both sides, and then by 3, tan theta cannot equal 1/3. Make sense?

OpenStudy (anonymous):

The tangent describes the ratio between the sine of an angle and the cosine of an angle. This cannot equal 1/3, so the sine of theta cannot equal the cosine of theta. Think about what the cosine and sine of an angle look like in terms of polar co-ordinates and you will see what this means for the graph.

OpenStudy (anonymous):

so the graph is undefined for theta=arctan(1/3) and will have no points corresponding to that angle?

OpenStudy (anonymous):

@dpaInc ??

OpenStudy (anonymous):

still trying to understand the problem of why \(\large \theta=arctan(1/3) \) "will have no effect".... what do you mean by this?

OpenStudy (anonymous):

im not sure .. the graph is is a linear line with cartesian equation y=1/3x+2/3 so what does the restriction actually mean?

OpenStudy (anonymous):

i do see that the theta restriction is put on the polar equation, but i don't know what that restriction did (or didn't do) on its cartesian form...

OpenStudy (anonymous):

so what effect does the restriction have on the shape of the graph?

OpenStudy (anonymous):

i'm thinking a hole in the linear graph.... but i'm not sure....

OpenStudy (anonymous):

the graph of cartesian has the same shape as its polar form yeah

OpenStudy (anonymous):

i'm not sure of the cartesian coordinates of the hole... if it is even a hole...

OpenStudy (anonymous):

yeah...

OpenStudy (anonymous):

so is it a hole?

OpenStudy (anonymous):

that's what i'm thinking... but idk exactly the cartesian coordinates of that hole.... (discontinuity)

OpenStudy (anonymous):

a removable discontinuity....

OpenStudy (anonymous):

i have another one.. parabola this time

OpenStudy (anonymous):

do i just say discontinuity at that angle

OpenStudy (anonymous):

yeah.. that's what i'd say.... hole or discontinuity... same thing...

OpenStudy (anonymous):

but if you say discontinuity, i think it would be more precise if you say removable discontinuity.

OpenStudy (anonymous):

but should the linear graph be continuous?

OpenStudy (anonymous):

shouldnt*

OpenStudy (anonymous):

ok.... i'm being more confident now that you're asking these questions that it is a hole.....

OpenStudy (anonymous):

the polar equation has a restriction that \(\large \theta \ne arctan(\frac{1}{3}) \), but overall, the graph is just a line

OpenStudy (anonymous):

does it have something to do with the fact that the tan(t)=1/3 for the graphs gradient?

OpenStudy (anonymous):

i think it has more to do with doing the conversion (or simplification)... take this for example..... if you were to graph \(\large y=\frac{(x+1)(x-1)}{(x+1)} \), you would get the same thing as graphing y = x-1 BUT in the first equation there is a hole at x=-1 while in the second graph there is no hole.

OpenStudy (anonymous):

oh is that like the limit

OpenStudy (anonymous):

and another queston.. 4y=x^2 i converted into polar and got r=4sin(t)/(cos(t))^2 = 0 . however i tried solving on calculator and got that as well as r=0? where did the r=0 come from

OpenStudy (anonymous):

no... i'm just talking about simplifying equations... like you did when you "simplified" or converted from polar form to cartesian form.... in polar form, you had a restriction, but the actual graph it looks like is a regular line with one exception... it has a hole....

OpenStudy (anonymous):

hang on.... lemme try...

OpenStudy (anonymous):

ok... i got the same as you but where did the "= 0" come from?

OpenStudy (anonymous):

the conversion from cartesian to polar is \(\large r=\frac{4sin\theta}{cos^2 \theta} \)

OpenStudy (anonymous):

and theres a restriction when cos^2theta=0 so when theta=pi/2,3pi/2 is there also discontrinuity at these agnles

OpenStudy (anonymous):

well, r=0 when \(\large \theta =2n\pi \), when n is an integer only... but when n is not that, then \(\large r\ne0 \)

OpenStudy (anonymous):

discontinuity at the polar graph but in the equation 4y=x^2, there is no discontinuity

OpenStudy (anonymous):

alright thanks for your help

OpenStudy (anonymous):

yw...

OpenStudy (anonymous):

another queston if you dont mind.. limacons have the form r=b+acos(theta) "If b>=2a, the limaçon is convex. If 2a>b>a, the limaçon is dimpled. If b=a, the limaçon degenerates to a cardioid. " why does the limacon go from dimpled to convex as b becomes >=2a? why does the 'dimple' disappear from as it exceeds 2a? can you explain in terms of the graph of r against theta?

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