Solving Sinusoidal Equations with Theta

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    Sinusoidal Theta
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SUMMARY

The forum discussion focuses on solving the equation ##\sin{\theta}\cos{\theta}=0.14##, with participants sharing methods to derive the angle ##\theta##. Key techniques include using the identity ##\sin(2\theta)=2\sin{\theta}\cos{\theta}## and the quadratic form of ##\tan{\theta}##. Participants also discuss the application of projectile motion equations to find ##\theta##, specifically using the relationship between horizontal distance and height in projectile motion. The final calculations yield angles of approximately 8.131° and 81.869°.

PREREQUISITES
  • Understanding of trigonometric identities, particularly ##\sin(2\theta)## and ##\tan{\theta}##.
  • Familiarity with projectile motion equations, including horizontal and vertical motion components.
  • Ability to manipulate equations involving inverse trigonometric functions, such as ##\arcsin{}##.
  • Proficiency in using a scientific calculator for trigonometric calculations.
NEXT STEPS
  • Learn how to derive and apply the identity ##\sin(2\theta)=2\sin{\theta}\cos{\theta}## in various contexts.
  • Study the kinematic equations for projectile motion to understand their derivation and application.
  • Explore the use of quadratic equations in trigonometric contexts, particularly in solving for angles.
  • Practice using scientific calculators for trigonometric functions, focusing on the arcsine function.
USEFUL FOR

Students preparing for physics exams, mathematicians solving trigonometric equations, and anyone interested in the application of trigonometry in projectile motion scenarios.

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Homework Statement
How much is the minimum angle at wich a football thrown by a striker has to come out if he wants to save a 1,9 m player barrier that are located at a distance of 11 m, if you hit the ball with a initial speed of 100 km/h?
Relevant Equations
##v_x=v_0\cos{\theta}=d/t##
##v_y=v_0\sin{\theta}-gt##
I can't solve ##\sin{\theta}\cos{\theta}=0,14##
Thanks!
 
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mcastillo356 said:
I can't solve ##\sin{\theta}\cos{\theta}=0,14##
Thanks!
Neither can I, but half a dozen tries on my calculator yielded 8.131°, equivalently 81.869°, both good to 4 digits. :wink:
 
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How did you get the relation
\sin\theta \cos\theta = 0.14? I got a quadratic equation of ##tan\theta##.
 
Haven't verified the physics, but you can use this:
$$\sin x\cos x=\frac 12\sin2x$$
You can find these identities using:
$$\cos x=\frac{e^{ix}+e^{-ix}}{2}$$$$\sin x=\frac{e^{ix}-e^{-ix}}{2i}$$
where ##i^2=-1##.
For your case, I just multiplied both functions.
 
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anuttarasammyak said:
How did you get the relation
\sin\theta \cos\theta = 0.14? I got a quadratic equation of ##tan\theta##.
##2\sin(\theta)\cos(\theta)=\sin(2\theta)=\frac{2t}{1+t^2}##, where ##t=\tan(\theta)##.
Also, ##\cos(2\theta)=\frac{1-t^2}{1+t^2}## and so ##\tan(2\theta)=\frac{2t}{1-t^2}##.
These formulae are worth remembering (I remember very few).
 
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Hi anuttarasammyak, Tom.G. archaic, the problem is that I can't manage with the scientific calculator. I already know the formulae you've given. which steps must I make to do it on my own?
It's this way
##v_x=v_0\cos{\theta}=d/t##
##v_y=v_0\sin{\theta}-gt##
On top of parabolic movement, ##v_y=0##
##v_0\sin{\theta}=gt##, so ##\sin{\theta}=gt/v_0##
Clearing ##t## from ##v_x## equation
##\sin{\theta}=\dfrac{g\cdot{d}}{v_0^2\cdot{\cos{\theta}}}##; so
##\sin{\theta}\cos{\theta}=\dfrac{g\cdot{d}}{v_0^2}##
Let's see if I've done the wright the LaTeX; I can't seem to preview
haruspex, the formulae you've given are fantastic, but, how can I manage to obtain ##\theta## with the scientific calculator?
 
mcastillo356 said:
Hi anuttarasammyak, Tom.G. archaic, the problem is that I can't manage with the scientific calculator. I already know the formulae you've given. which steps must I make to do it on my own?
It's this way
##v_x=v_0\cos{\theta}=d/t##
##v_y=v_0\sin{\theta}-gt##
On top of parabolic movement, ##v_y=0##
##v_0\sin{\theta}=gt##, so ##\sin{\theta}=gt/v_0##
Clearing ##t## from ##v_x## equation
##\sin{\theta}=\dfrac{g\cdot{d}}{v_0^2\cdot{\cos{\theta}}}##; so
##\sin{\theta}\cos{\theta}=\dfrac{g\cdot{d}}{v_0^2}##
Let's see if I've done the wright the LaTeX; I can't seem to preview
haruspex, the formulae you've given are fantastic, but, how can I manage to obtain ##\theta## with the scientific calculator?
$$\frac 12\sin2x=0.14\implies2x=\arcsin{0.28}\implies x=\frac12\arcsin{0.28}$$
This will give a value of ##x## in ##[-\pi/2,\,\pi/2]##.
The arcsine function is available in scientific calculators.
 
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The best way is without a doubt @archaic's. You could also try
$$\sin^2 \theta \cos^2 \theta = \sin^2 \theta (1-\sin^2 \theta) = 0.14^2$$ and let ##u = \sin^2 \theta## to get a quadratic in ##u##.
 
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Hi, archaic, forum
My calculator gives 8,13010... degrees. Correct?
 
  • #10
mcastillo356 said:
It's this way
Where in your way "1,9 m player barrier" is considered ?
 
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  • #11
Hi, anuttarasammyak
Not at all. Strange, isn't it?
It's all about an already solved problem by the spanish UNED. I'm preparing the access exam previous to get matriculated on the grade of maths
 
  • #12
I am afraid you have a wrong solution. For hobbit barriers and for Godzilla barriers you kick the ball at the same angle ? You had better ask it to your teacher.
 
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  • #13
Haha...!. Yes indeed...!. I will try to solve it my way. I'm back today. Now it's 12.24 PM in Spain. Please, forum, give me time
 
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  • #14
mcastillo356 said:
On top of parabolic movement,
You cannot assume that is where it must be at 1,9m.
Even if the question were to find the minimum launch velocity to clear the player that would not be a correct assumption.
 
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  • #15
haruspex said:
You cannot assume that is where it must be at 1,9m
It might be the case that the universe (and the data given) conspire and the peak of that parabola lies exactly 1.9m above the ground...
 
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  • #16
haruspex said:
##2\sin(\theta)\cos(\theta)=\sin(2\theta)=\frac{2t}{1+t^2}##, where ##t=\tan(\theta)##.
Also, ##\cos(2\theta)=\frac{1-t^2}{1+t^2}## and so ##\tan(2\theta)=\frac{2t}{1-t^2}##.
These formulae are worth remembering (I remember very few).
Also it is an other important formula worth remembering:
$$\frac{1}{\cos^2(\theta)}=1+\tan^2(\theta)$$
With this one, you get a quadratic equation in theta.
 
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  • #17
I've written to my teacher. Let's see what says.
 
  • #18
Thanks berkeman!.
 
  • #19
mcastillo356 said:
I've written to my teacher. Let's see what says.
Why? Let's just try to solve it correctly.
You know that after traveling x=11m horizontally it needs to be at height y=1,9m.
Suppose it takes time t to get there.
If you kick it at speed v and at angle theta above the horizontal, what will x and y be at time t?
What two equations does that allow you to write?
 
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  • #20
Hi haruspex!
I've already done it by myself: it's ##0,09\pi##rad
 
  • #21
mcastillo356 said:
Hi haruspex!
I've already done it by myself: it's ##0,09\pi##rad
Seems too much. Please post your working.
 
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  • #22
I think that things missing, I mean, the distance, for example, is at the statement of the problem; the height of the barrier is implicit in ##\sin{\theta}## and ##\cos{\theta}##. So:
mcastillo356 said:
##v_x=v_0\cos{\theta}=d/t##
##v_y=v_0\sin{\theta}-gt##
On top of parabolic movement, ##v_y=0##
##v_0\sin{\theta}=gt##, so ##\sin{\theta}=gt/v_0##
Clearing ##t## from ##v_x## equation
##\sin{\theta}=\dfrac{g\cdot{d}}{v_0^2\cdot{\cos{\theta}}}##; so
##\sin{\theta}\cos{\theta}=\dfrac{g\cdot{d}}{v_0^2}##

archaic said:
$$\frac 12\sin2x=0.14\implies2x=\arcsin{0.28}\implies x=\frac12\arcsin{0.28}$$
This will give a value of ##x## in ##[-\pi/2,\,\pi/2]##.
The arcsine function is available in scientific calculators.

And then:
##\arcsin{0,28}=16,26## degrees;
Degrees to radians:
##\dfrac{16,26º\pi\mbox{rad}}{180º}=0,09\pi\mbox{rad}##

Pros and cons:
Am I talking to myself?; 16,26 are degrees?; what the hell is this diabolic statement of the problem?;
On the other hand: the result is more than ##-2\pi## and less than ##2\pi##

haruspex said:
Seems too much

Yes:confused:
 
  • #23
mcastillo356 said:
I think that things missing, I mean, the distance, for example, is at the statement of the problem; the height of the barrier is implicit in ##\sin{\theta}## and ##\cos{\theta}##. So:

And then:
##\arcsin{0,28}=16,26## degrees;
Degrees to radians:
##\dfrac{16,26º\pi\mbox{rad}}{180º}=0,09\pi\mbox{rad}##

Pros and cons:
Am I talking to myself?; 16,26 are degrees?; what the hell is this diabolic statement of the problem?;
On the other hand: the result is more than ##-2\pi## and less than ##2\pi##
Yes:confused:
Your answer is wrong. As I pointed out in post #14, you cannot assume that 1,9m is the top of the arc.

Instead, follow the system I laid out in post #19.
 
  • #24
A useful shortcut for projectile motion questions like this is the general form of the parabolic trajectory $$y = x\tan{\theta} - \frac{gx^2}{2u^2 \cos^2{\theta}}$$although I wouldn't use it unless you can derive it first. It comes from combining the two equations for ##x(t)## and ##y(t)## w/ uniform acceleration of magnitude ##g## in the ##-\hat{y}## direction.
 
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  • #25
Here is the image of the parabolic movement. Excuse my spanglish ("parabolic movement" is the words for this image?)
20200621_011715.jpg
 
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  • #26
Ooops... Hope not to done something not allowed
 
  • #27
Like @haruspex mentioned, you can't assume that the ball crosses the barrier at the highest point of its trajectory. You are expecting solutions that look something like this:

1592696086917.png


Generally you will have 2 distinct solutions for ##\theta##, corresponding to each trajectory. Only if these both happen to be the same will highest point on the trajectory be at the barrier.
 
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  • #28
Wow...!. It's true... It might travel to the Moon and save the barrier, and score
 
  • #29
haruspex said:
Why? Let's just try to solve it correctly.
You know that after traveling x=11m horizontally it needs to be at height y=1,9m.
Suppose it takes time t to get there.
If you kick it at speed v and at angle theta above the horizontal, what will x and y be at time t?
What two equations does that allow you to write?

Maybe ##v_f^2=v_i^2-2g\Delta{y}##
##\Delta{x}=v_o\cos{\theta}\cdot{t}##
No
 
  • #30
Tomorrow I will try once again. It's 02:08 AM.:sleep:
 

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