salman213 said:
sketch the curve with the given vector equation...
r(t) = (sint)i + (sint)j + squareroot(2)(cost)k
Hmm...
r(t) = | sin(t) |
| sint(t) |
| sqrt(2)cos(t) |
Yes, ok.
The above equation represents the possition vector of a point on the curve with respect to a varible t. In this case, the i and j components will always be equal in magnitude;
So if we draw our axis;
j | /
| /
| /
| /
|/_______________ i
Then our resultant diagonal is the result. Now if you imagine that diagonal line as a sheet of paper perpendicular to your computer screen this represents the k axis.
We will no concern outselves with what that looks like;
i or j |
|
|
|
|_____________ k
Because both the i and j components are the same, it doesn't matter which we are using to describe the resultant curve. We can actually call that axis the i-j plane and treat is as another set of axis (note: can't do this if the i-j plane was a curve)
Hence with respect to this 2D axis we have;
r(t) = (sint)j + sqrt(2)(cost)k
Now if t is an angular quantatity as in normal polar co-ordinates (messured anti-clockwise from the positive k axis).
Then as;
t = 0, k = sqrt(2) as cos(0) = 1, as
t = 1/2pi, sin(t)i = 1 and sin(t)j = 1 => The magnitude of this vector point in the i-j plane is sqrt( 1
2 + 1
2) which is the same as sqrt(2).
Hence can you see that it describes a circular motion in three dimentions?
The circle is being described in the i-j plane, by the k componant of the vector. Sorry that's not a very clear mathamatical way of showing it, but hopefully it will help you visulise what r(t) is. Once you can do that, it shouldn't be too hard to understand that in three diemensions a circle is just a 'hoop' that fits around a sphere in all three directions of rotation. And hence it 'lies on the [imaginary] sphere.
As you should know, that x
2i + y
2j + z
2k = r
2 describes a sphere, then it doesn't take a lot to compare your two equations and their co-effs.
I hope that helps,
Haths