If your solution to stated problem does not match the given solution, you should self-critique per instructions at
http://vhcc2.vhcc.edu/dsmith/geninfo/labrynth_created_fall_05/levl1_22/levl2_81/file3_259.htm
.
Your solution, attempt at solution. If you are unable to attempt a solution, give a phrase-by-phrase interpretation of the problem along with a statement of what you do or do not understand about it. This response should be given, based on the work you did in completing the assignment, before you look at the given solution.
qa 10_5
No q_a_ appears to be necessary for this section. You may proceed to the section and the problem assignment.
The problem assignment is repeated here for your convenience:
Section 10.5
1) Find the tangential and normal components of an object's acceleration which has the position vector R(t) = <2 cos t, 5 sin t>.
2) Find the tangential and normal components of an object's acceleration which has the position vector R(t) = <3/5 cos t, 4/5(1+sin t), cos t>.
3) If V(0) = -2i - 3j and A(0) = 2i + 3j, what is A_T and A_N at t = 0?
4) If V(0) = <5,-2,4> and A(0) = <1,3,-9>, what is A_T and A_N at t = 0?
5) ||V|| = sqrt(e^-t + t^4). What is A_T at t = 0?
6) Where on the trajectory of R(t) = <2t^2 - 5t, 5t + 2, 4t^2> is the speed maximized and minimized?
7) An object moves with a constant angular velocity omega around the circle x^2 + y^2 = r^2 in the xy-plane.
8) A car which weighs 3,000lbs moves along the elliptic path 1600x^2 + 100y^2 = 1, where x and y are measured in miles. If the car travels at the constant speed of 30mi/hr, how much frictional force is required to keep it from skidding as it turns at (1/40,0)? What about at (0,1/10)?
9) ** Consider the vector function R(t) = <3 sin t, 4t, 3 cos t>.
10) ** Use the method described in the previous problem to find A_T and A_N for R(t) = <cos t, sin t>.
11) ** Let B = T X N when T and N are the unit tangent and normal vectors to a curve C with position vector R. Show that dB/ds = T X (dN/ds).
12) An object connected to a string of length r is spun counterclockwise in a circular path in a horizontal plane. Let omega be the constant angular velocity of the object.