Expression for the instantaneous angular velocity

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Rahulrj
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Homework Statement


The directed beam from a small but powerful searchlight placed on the ground tracks a small plane flying horizontally at a fixed height h above the ground with a uniform velocity v. If the search light starts rotating with an instantaneous angular velocity ##\omega_0## at time ##t=0## when the plane was directly overhead, then at a later time t, its instantaneous angular velocity ##\omega(t)## is given by?

Homework Equations


##\omega## = ##\omega_0##+##\alpha t##
##\omega^2## = ##\omega_0^2## + 2##\alpha \theta##
##\theta## = ##\omega_0 t##+1/2##\alpha t^2##

The Attempt at a Solution


I am not sure where to begin the solution other than the equations I have written above.
The answer given is ##\frac{\omega_0}{1+\omega_0^2t^2}##. I tried differentiating but I don't seem to get anywhere with it.
 
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Rahulrj said:

Homework Statement


The directed beam from a small but powerful searchlight placed on the ground tracks a small plane flying horizontally at a fixed height h above the ground with a uniform velocity v. If the search light starts rotating with an instantaneous angular velocity ##\omega_0## at time ##t=0## when the plane was directly overhead, then at a later time t, its instantaneous angular velocity ##\omega(t)## is given by?

Homework Equations


##\omega## = ##\omega_0##+##\alpha t##
##\omega^2## = ##\omega_0^2## + 2##\alpha t##
##\theta## = ##\omega_0 t##+1/2##\alpha t^2##

The Attempt at a Solution


I am not sure where to begin the solution other than the equations I have written above.
The answer given is ##\frac{\omega_0}{1+\omega_0^2t^2}##. I tried differentiating but I don't seem to get anywhere with it.
You tried differentiating - what?
ω need not be either a linear or quadratic function of time.
Make a picture, and everything will be clear.
How does the angle theta depend on time? How is the angular velocity ω defined?
upload_2017-5-16_9-44-10.png
The blue line represent the light beam at t=0, the red line is the light beam at a later time t.
 
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ehild said:
You tried differentiating - what?
ω need not be either a linear or quadratic function of time.
Make a picture, and everything will be clear.
How does the angle theta depend on time? How is the angular velocity ω defined?
View attachment 203608The blue line represent the light beam at t=0, the red line is the light beam at a later time t.
That to an extent was helpful however embarrassing to me I still couldn't get the right answer.
I took sine of the angle theta, so ##\sin\theta = vt/l## where l is the line connecting the searchlight and the plane
##\theta = \sin^{-1}(vt/l)## I used ##v = l\omega## to make the substitution in vt/l
differentiating it I get##\omega = \frac{\omega}{\sqrt{1-\omega^2t^2}}##
 
Rahulrj said:
That to an extent was helpful however embarrassing to me I still couldn't get the right answer.
I took sine of the angle theta, so ##\sin\theta = vt/l## where l is the line connecting the searchlight and the plane
##\theta = \sin^{-1}(vt/l)## I used ##v = l\omega## to make the substitution in vt/l
differentiating it I get##\omega = \frac{\omega}{\sqrt{1-\omega^2t^2}}##
l is changing, use vt/h = tan (theta) instead.
 
ehild said:
l is changing, use vt/h = tan (theta) instead.
I did use Tan at first however I got an answer with the terms l and h which couldn't figure out a way to eliminate. So with tan I get
##\theta = \tan^{-1}{vt/h}##
on differentiating I get ## \omega = \frac{\omega }{h/l+l\omega^2t^2/h}##
and I do not know how to simplify it further hence I used sine in my previous post
 
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Rahulrj said:
I did use Tan at first however I got an answer with the terms l and h which couldn't figure out a way to eliminate. So with tan I get
##\theta = \tan^{-1}{vt/h}##
on differentiating I get ## \omega = \frac{\omega }{h/l+l\omega^2t^2/h}##
and I do not know how to simplify it further hence I used sine in my previous post
That doesn't make much sense. Did you mean ω0 on the right?
Please post your working.
 
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Rahulrj said:
I did use Tan at first however I got an answer with the terms l and h which couldn't figure out a way to eliminate. So with tan I get
##\theta = \tan^{-1}{vt/h}##
on differentiating I get ## \omega = \frac{\omega }{h/l+l\omega^2t^2/h}##
and I do not know how to simplify it further hence I used sine in my previous post
I don not follow you.
You have ##\theta = \tan^{-1}({vt/h})##
Differentiate it with respect to t. What do you get? Remember v and h are constants.
 
ehild said:
I don not follow you.
You have ##\theta = \tan^{-1}({vt/h})##
Differentiate it with respect to t. What do you get? Remember v and h are constants.
Differential of ##Tan^{-1}x = \frac{1}{1+x^2}##
so then ##\omega = (1/1+(vt/h)^2 )* v/h##
substituting ##v=l\omega##
##\omega = 1/1+(l\omega t/h)^2 * v/h##
and I end up with ## \omega = \frac{\omega }{h/l+l\omega^2t^2/h}##

I found where I made mistake 'v' should be, ##v=h\omega_0##
and with that substitution
I get the answer ## \omega = \frac{\omega_0}{1+\omega_0^2t^2}##
 
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Rahulrj said:
Differential of ##Tan^{-1}x = \frac{1}{1+x^2}##
so then ##\omega = (1/1+(vt/h)^2 )* v/h##

correct so far...
Rahulrj said:
substituting ##v=l\omega##
That is wrong. You've just derived the expression for ω, it is not v/L.
You have to find ω0, the angular velocity at t=0. Substitute t=0 into the equation for ω, what do you get?
 
ehild said:
correct so far...

That is wrong.
You have to find ω0, the angular velocity at t=0. Substitute t=0 into the equation for ω, what do you get?
Seems like you did not see my update in post #8.
 
Rahulrj said:
Seems like you did not see my update in post #8.
Well, I did not see. You got it at last!
Next time remove the wrong part from your post.
 
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