Math 6C – Exam
2 – Fall 2002
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1. Find a unit
vector in the direction of ( 2, 5 ). The y–component equals what?
Just divide
this vector by it’s length, and you have a unit vector
in the same direction:

The
y-component of this vector is thus 
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2. A = (–3, 1) and B = (2, 5).
The vector projection of A onto B has x–component equal to what?
The vector projection of A onto B is given by:

The x-component
of this projection vector is thus
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3. A = (3, –2, 1) and B = (–1, 2, 5). Find a unit vector in the direction of B x A.
Its x–component
equals what?

Now divide this vector by its length:

The
x-component of this vector is thus
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4. a(t) = (p sin(pt), 5t4) , v(0)
= (1,0), r(0) = (0,1).
Then what is the y-component
of r(1) ?

Use the given initial condition
to solve for the two constants of integration:

And now we integrate again to
find the position as a function of time:
.
Use the given initial condition
to solve for the two constants of integration:
.
.Hence, the y-component of r(1) is
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5. Find the unit tangent vector T
for the plane curve r(t) = (sin
(2t), e3t). The
absolute value of the x–component of
T is what?


And the
absolute value of the x-component of T is thus
.
6. Find the principal unit normal vector N for
the plane curve r(t) = (sin
(2t), e3t). The
absolute value of the x–component of
N is what?
In problem #5 we found that
.
The principal unit normal
vector for this curve is given by
.
,

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7. Find the principal unit binormal
vector B for the plane curve r(t) = (sin (2t),
e3t). The absolute value of the x–component of B
is what?
Simply realize that since this is a plane curve were T and N are always in the xy-plane, B must always be perpendicular to the xy-plane, so B =
(0,0,1)! J
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8. Find the curvature, k,
for r(t) = (sin
(2t), e3t) at t = p.




And so

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9. Find the radius of curvature (the
radius of the osculating circle) of ![]()
at the point (0, 1).
Since the given parabolic curve
is symmetric about the y-axis, and the given point is on the y-axis, it follows
that the best-fit circle has its center on the y-axis. Suppose the center is (0,c). Then the equation of the osculating circle is
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hence
Thus the osculating circle is
given by
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The slope of the circle at (0,
1) is 0 (since the cosine has a horizontal tangent line there). Implicitly differentiating the above
equation with respect to x, we get:

The first derivatives of the
cosine and this circle are both 0 at x=0.
The second derivative of the cosine is negative the cosine, so at x=0 is
–1, which needs to also be the second derivative of the osculating circle at
(0, 1).

,
and
since this must equal –1, we have
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Thus, the radius of curvature is
![]()
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10. Find length of the parametrized curve,
from (Just
write down the integral that equals this arclength,
but don’t solve it!) |
|
, so

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11. Find cosine of the angle between the velocity and acceleration vectors of
at t=0. |
|
,
hence
.

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12. Find the
velocity and acceleration for the space curve
|
|

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13. Find the (smaller) angle (in radians) between
velocity and acceleration vectors of the space curve
, at t=0.
Substitute t=0 into the results
of #12:

Then

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14. Find the curvature of the space curve
at t=0.

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15. Find the torsion of the space curve
at t=0.

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