How Do Physics and Trigonometry Intersect in Simple Motion Problems?

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The discussion focuses on the intersection of physics and trigonometry in solving simple motion problems. The first problem involves determining the landing position of a mass rolled off a table, with the correct trajectory described as a downward concave parabola, confirmed by resolving the equations of motion. The second problem addresses the amplitude and phase of a trigonometric expression, yielding correct values for both. The third problem highlights the relationship between coefficients in a trigonometric identity, revealing the importance of sign in determining the correct phase angle. The participants emphasize the need to consider the signs of the coefficients when rewriting expressions, as this affects the resulting phase angle and amplitude.
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Just wanting to double check the reasoning and the work for these. They are fairly simple, so I didn't use latex, but I can re-edit at any time if someone so desires (I'm online more often than I like to admit hehehe).

Thanks.

Homework Statement


1) A mass 'm' is rolled of a table at height 'h' with horizontal speed 'Vx'. Where does the mass land? What trajectory did the mass take?

2) If x = -cos(t) + 3*sin(t), what is the amplitude and phase?

3) Show that an equivalent expression for x = C1 * cos(wt) + C2 * sin(wt) is B*cos(wt + P). How do B and P depend on C1 and C2.


Homework Equations


1) F = ma
2) sin(a +- b) = sin(a)cos(b) +- cos(a)sin(b)
3) cos(a +- b) = cos(a)cos(b) -+ sin(a)sin(b)


The Attempt at a Solution



1) I solved the equations of motion for both vertical and horizontal directions.
With y(0) = h and Vy(0) = 0, I got y(t) = h - mg/2 * t^2

With x(0) = 0 and Vx(0) = Vx, I got x(t) = Vx * t

Solving for y = 0, t_land = sqrt(2/[mg]), so I said the mass will have fallen and displaced Vx * t_land away from table.

Plugging x/Vx for 't', I have that the path is y(t) = h - mg/2 * (x/Vx)^2, which is a parabola with downward concavity.

2) If we rewrite as A * sin(wt + P), then A * sin(P) = C1 and A * cos(P) = C2
Therefore A is simply sqrt(C1^2 + C^2) = sqrt(10).
and P = arctan(C1/C2) = arctan(-1/3).

3) If we rewrite as B * cos(wt + P), then B * cos(P) = C1 and - B * sin(P) = C2
Therefore B is simply sqrt(C1^2 + C^2)
and P = arctan(-C2/C1)
 
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Err, I know it's not exactly challenging, but if anybody could take a look and tell me if it's right, that would be cool (especially for #1, the others I'm 100% are correct, not even sure why I posted them).
 
end3r7 said:
1) I solved the equations of motion for both vertical and horizontal directions.
With y(0) = h and Vy(0) = 0, I got y(t) = h - mg/2 * t^2
That "m" doesn't belong there. Resolve for t and you're good to go.

The other two problems look OK.
 
Doc Al said:
That "m" doesn't belong there. Resolve for t and you're good to go.

The other two problems look OK.

Wow, thanks a lot.

After the proper fixing, I got that the time for landing is T = sqrt(2h/g)
x will have displaced by Vx * T.

The equation, in terms of x is y(x) = h - g/2 * (x/Vx)^2, with x ranging from 0 to Vx * T. The equation describing the right half of a parabola with downward concavity.
 
Looks good.
 
I have a question though, for 3, say I use x = -cos(2t) + 3*sin(2t) and try to write it as y = B*cos(2t+P)

Then I use B is simply sqrt(10)
and P = arctan(3)

This is giving me an error though. x = -y.

Why is that?

I know it's because B is in fact -sqrt(10), but how can we determine that?
 
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Oops. I think you made an error in #3 before:

end3r7 said:
3) If we rewrite as B * cos(wt + P), then B * cos(P) = C1 and - B * sin(P) = C2
Therefore B is simply sqrt(C1^2 + C^2)
and P = arctan(-C2/C1)
Redo your answer for P. (One difference between #2 & #3 is that one uses Sin(wt +P) while the other uses Cos(wt + P) )
 
Doc Al said:
Oops. I think you made an error in #3 before:


Redo your answer for P. (One difference between #2 & #3 is that one uses Sin(wt +P) while the other uses Cos(wt + P) )


I thought the P was right...

The B was wrong by a factor of -1.

This is because when we solve for B we get +or-sqrt(C1^2 + C2^2).

For the first case, we got the positive square root, but this time around we need the negtavie, I'm wondering why.
 
A change in sign is equivalent to a change in P. If you choose B as positive (amplitudes are always positive), that determines P.
 
  • #10
Which step was wrong for the solving for P then? I'm a little confused.

I understand that I could as easily keep my B positive and shift the argument inside the cosine function by adding pi, but I would rather not, unless there is a clear motivation in the equations.
 
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  • #11
I think the problem is that (as you pointed out) this method gives a choice of +/- for B. To see which fits a particular case, you must plug in the values. (Interesting!)

Note that:
\tan(\theta + \pi) = \tan\theta

But:
\cos(\theta + \pi) = -\cos\theta
 
  • #12
I figured out why. When we foud P, we took the arctan which returns an angle between -pi /2 and pi/2, where cosine is never negative.

Thus if we have c1 = Bcos(P), then a negative c1 would imply that we need to take the negative square root.
 
  • #13
Good. Another way of looking at it is what I tried to explain above. Arctan(x) gives an angle which is ambiguous by an additive term of \pm\pi radians.
 
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