polar graph restriction
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
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?
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.
so the graph is undefined for theta=arctan(1/3) and will have no points corresponding to that angle?
@dpaInc ??
still trying to understand the problem of why \(\large \theta=arctan(1/3) \) "will have no effect".... what do you mean by this?
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?
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...
so what effect does the restriction have on the shape of the graph?
i'm thinking a hole in the linear graph.... but i'm not sure....
the graph of cartesian has the same shape as its polar form yeah
i'm not sure of the cartesian coordinates of the hole... if it is even a hole...
yeah...
so is it a hole?
that's what i'm thinking... but idk exactly the cartesian coordinates of that hole.... (discontinuity)
a removable discontinuity....
i have another one.. parabola this time
do i just say discontinuity at that angle
yeah.. that's what i'd say.... hole or discontinuity... same thing...
but if you say discontinuity, i think it would be more precise if you say removable discontinuity.
but should the linear graph be continuous?
shouldnt*
ok.... i'm being more confident now that you're asking these questions that it is a hole.....
the polar equation has a restriction that \(\large \theta \ne arctan(\frac{1}{3}) \), but overall, the graph is just a line
does it have something to do with the fact that the tan(t)=1/3 for the graphs gradient?
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.
oh is that like the limit
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
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....
hang on.... lemme try...
ok... i got the same as you but where did the "= 0" come from?
the conversion from cartesian to polar is \(\large r=\frac{4sin\theta}{cos^2 \theta} \)
http://www.wolframalpha.com/input/?i=solve+%284rsin%28theta%29%3Drcos^2%28theta%29+for+r they got r=0 as well
and theres a restriction when cos^2theta=0 so when theta=pi/2,3pi/2 is there also discontrinuity at these agnles
well, r=0 when \(\large \theta =2n\pi \), when n is an integer only... but when n is not that, then \(\large r\ne0 \)
discontinuity at the polar graph but in the equation 4y=x^2, there is no discontinuity
alright thanks for your help
yw...
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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