Classical Mechanics - Problem Set 1 with Solutions | PHYS 3610, Assignments of Mechanics

Material Type: Assignment; Class: Classical Mechanics; Subject: PHYS Physics; University: Tennessee Tech University; Term: Fall 2008;

Typology: Assignments

Pre 2010

Uploaded on 07/30/2009

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Phys 3610, Fall 2008
Problem Set #1, Hint-o-licious Hints
1. Taylor,1.18 Recall that the area of a triangle follows the basic formula
Area = 1
2(base)(height)
and use the fact that
a×b=|ab sin θ|
where θis the angle between aand b.
2. Taylor,1.28 Now there are forces between particles 1 and 2, 2 and 3, and 1 and 3.
3. Taylor,1.36 More review of 2110 kinematics problems. Got to remember the old stuff
before we move on to the new stuff!
4. Taylor,1.37 This is a review of free-body diagrams and basic acceleration problems from
2110. The net force on the puck must be directed down the slope. Find its acceleration and
solve for the it takes to come back to x= 0.
5. Taylor,1.45 Take
d(r2)
dt =d(r·r)
dt
6. Taylor,2.8 Look over the (easy) theorem in Problem 2.7 and just follow the formula for
the F(v) that is given. The answer for v(t) is not an exponential, but a power law of sorts.
At alrge t,vgoes like 1/t2.
7. Taylor,2.17 This is fairly simple algebra. Use (2.36a) directly in the first term of (2.36b)
and from (2.36a) solve for tin terms of xthen use that result in the second term of (2.36b).
(2.37) then comes out pretty directly.
8. Taylor,2.19 The first part has you re-derive the 2110 result, which you probably should
(don’t just look it up) because you don’t teach it every year like I do. Express the result
(that is, yas a function of x) in terms of vx0and vy0.
For the second part, use the Taylor expansion of ln(1 ) for small given in (2.40) in
the second term of (2.37). (Why is this expansion valid for the limit we are considering?)
1

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Phys 3610, Fall 2008 Problem Set #1, Hint-o-licious Hints

  1. Taylor, 1.18 Recall that the area of a triangle follows the basic formula

Area = 12 (base)(height)

and use the fact that a × b = |ab sin θ|

where θ is the angle between a and b.

  1. Taylor, 1.28 Now there are forces between particles 1 and 2, 2 and 3, and 1 and 3.
  2. Taylor, 1.36 More review of 2110 kinematics problems. Got to remember the old stuff before we move on to the new stuff!
  3. Taylor, 1.37 This is a review of free-body diagrams and basic acceleration problems from
  4. The net force on the puck must be directed down the slope. Find its acceleration and solve for the it takes to come back to x = 0.
  5. Taylor, 1.45 Take d(r^2 ) dt

d(r · r) dt

  1. Taylor, 2.8 Look over the (easy) theorem in Problem 2.7 and just follow the formula for the F (v) that is given. The answer for v(t) is not an exponential, but a power law of sorts. At alrge t, v goes like 1/t^2.
  2. Taylor, 2.17 This is fairly simple algebra. Use (2.36a) directly in the first term of (2.36b) and from (2.36a) solve for t in terms of x then use that result in the second term of (2.36b). (2.37) then comes out pretty directly.
  3. Taylor, 2.19 The first part has you re-derive the 2110 result, which you probably should (don’t just look it up) because you don’t teach it every year like I do. Express the result (that is, y as a function of x) in terms of vx 0 and vy 0. For the second part, use the Taylor expansion of ln(1 − ) for small  given in (2.40) in the second term of (2.37). (Why is this expansion valid for the limit we are considering?)