lLovePhysics said:
I have a question on the formulas for arc length and surface area.
Do you use the formula: s= \int_{c}^{d}\sqrt{1+[g'(y)]^2}dy only when you are provided with a function x=g(y)?? Can you convert that to y=g(x) and solve it by replacing g'(y) with y(x), changing the bounds and the dy to dx?
Yes, you can. In fact, if you have
both x and y as functions of some parameter t, say x= f(t), y= g(t) then s= \int \sqrt{f'(t)^2+ g'(t)^2}dt. That reduces your first integral if x= t, y= g(t) and to your second if x= f(t), y= t.
Like for example if you wanted to solve:
Find the area of the surface formed by revolving the graph of f(x)=x^2 on the interval [0,2] about the y-axis.
How would you know whether to find the surface area with respect to x or y? Are these independent on the axis of revolution? Why does the book give the Surface area formula with respect to x and y?
I'm not sure I understand your last question- you don't say what formula you are talking about.
If, for example, you had a straight line x= a, rotated around the y-axis, you would get a circular cylindar of radius a. Its surface area would be the circumference of the circle, 2\pi x= 2 \pi a time the height (measured in the y direction) h. For a curved figure rotated around the y-axis, you would, of course, imagine very thin "layers", each a very short cylinder, stacked on top of one another. In each cylinder, since x does not change MUCH, you can approximate the surface area by 2\pi x dy where "dy" is the height. The total surface area can be approximated by the Riemann sum \Sum (2\pi x dy) and can be made exact by the limit process that gives the integral 2\pi\int x dy. Of course, in the case that x= g(y) that becomes 2\pi\int g(y)dy. If the graph y= f(x) is rotated about the x-axis, that would, of course, just swap x and y ("of course" because you can just swap x and y in the "Riemann sum" argument): 2\pi\int ydx= 2\pi\int f(x)dx.
In both of those, the curve is rotated around the x or y axis. But you can use the same argument for any axis. Suppose you have the curve x= g(y) rotated around an axis x= a rather than the x-axis, x= 0. First you would draw a picture and decide whether the graph is on the left or right of x= a. That's important because the radius of the circle formed has to be positive: r= |x- a| which is either x- a or a- x depending upon whether x is larger than or less than a. (If the graph x= g(y) crosses the line x= a, you will need to do separate integrals for g(y)< a and g(y)> a.) If x> a, then the circle has radius x- a rather than just x and so the circumference is 2\pi (x- a) and the surface area integral becomes
\int 2\pi (x-a) dy= 2\pi \int (g(y)-a)dy.
Again, if you are given y= f(x) rotated around the line y= b, you just swap x and y: 2\pi\int |f(x)- b|dx.