Find the Value of θ in a Pulley Blocks Problem - Homework Solution

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Homework Help Overview

The problem involves determining the angle θ in a pulley system with moving blocks. The context suggests a focus on the dynamics of the system, particularly how the motion of the pulley affects the relationship between the blocks and the string.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the implications of the moving pulley on the velocities of the blocks and suggest different frames of reference for analysis. Some propose using geometric relationships and trigonometric identities to express the lengths involved, while others consider the effects of time increments on these lengths.

Discussion Status

There are multiple lines of reasoning being explored, including working in the frame of the pulley and applying virtual work methods. Participants have raised questions about the validity of their approaches and the treatment of variables, indicating an ongoing exploration of the problem without a clear consensus on the best method.

Contextual Notes

Some participants express uncertainty about the assumptions made regarding the motion of the blocks and the constraints of the string length. There are also mentions of potential sign errors and the treatment of coordinates versus distances in the analysis.

Tanya Sharma
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Homework Statement



Q. In the figure shown, find out the value of θ [ assume string to be tight ]

Homework Equations





The Attempt at a Solution



If the pulley was not moving ,then we could have equated the component of velocities of the two blocks along the string .

But,since the pulley is moving,something extra needs to be done .Not sure what .

I would be grateful if somebody could help me with the problem .
 

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Tanya Sharma said:

Homework Statement



Q. In the figure shown, find out the value of θ [ assume string to be tight ]

Homework Equations





The Attempt at a Solution



If the pulley was not moving ,then we could have equated the component of velocities of the two blocks along the string .

But,since the pulley is moving,something extra needs to be done .Not sure what .

I would be grateful if somebody could help me with the problem .

I am not sure but how about working in the frame of pulley?
 
Pranav-Arora said:
I am not sure but how about working in the frame of pulley?

Could you elaborate what do you mean by working in the pulley frame ? What benefit does it give in the context of the problem ?
 
Tanya Sharma said:
Could you elaborate what do you mean by working in the pulley frame ? What benefit does it give in the context of the problem ?

I meant that if you work in the frame fixed to the pulley, the blocks have an additional component of velocity downwards. You can then equate the velocity along the string. (And that gives one of the answers mentioned.)
 
I analyzed this a little differently. Drop a normal from the pulley to the line joining the tops of blocks A and B. Call the length of this normal h. You then have two right triangles. Express the other sides of these two right triangles trigonometrically in terms of h (using trig functions of 30 degrees and θ). Let a small increment of time Δt pass. Express then new sides of the two triangles in terms of Δt. The sum of the hypotenuses of these new triangles must be the length of the string, which is constrained to be unchanged. So set the sum of the new hypotenuses equal the sum of the original hypotenuses. Expand each of the two hypotenuses as a linear function of Δt. Certain terms will cancel from both sides of the equation. Set the coefficient of Δt equal to zero. Solve for θ, or substitute each of the possible answers into the equation, and see which one satisfies it.

Chet
 
Chestermiller said:
I analyzed this a little differently. Drop a normal from the pulley to the line joining the tops of blocks A and B. Call the length of this normal h. You then have two right triangles. Express the other sides of these two right triangles trigonometrically in terms of h (using trig functions of 30 degrees and θ). Let a small increment of time Δt pass. Express then new sides of the two triangles in terms of Δt. The sum of the hypotenuses of these new triangles must be the length of the string, which is constrained to be unchanged. So set the sum of the new hypotenuses equal the sum of the original hypotenuses. Expand each of the two hypotenuses as a linear function of Δt. Certain terms will cancel from both sides of the equation. Set the coefficient of Δt equal to zero. Solve for θ, or substitute each of the possible answers into the equation, and see which one satisfies it.

Chet

Hi Chet...

Sorry for the late response .

Let h be the length of the normal ; x length of the left string and y length of the right string ; a and b be the length of the bases of left and right triangles respectively at t=0.

x=hcosecθ and y=hcosec30°
a=hsecθ and b=hsec30°

Now after time Δt ,

a' = a-3.25Δt
h' = h+Δt
b' = b+√3t

Now x+y = √(a'2+h'2) + √(b'2+h'2)

[tex]hcosecθ+hcosec30° = \sqrt{(hsecθ-3.25Δt)^2+(h+Δt)^2} + \sqrt{(hsec30°+\sqrt{3}Δt)^2+(h+Δt)^2}[/tex]

Is it correct ?
 
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Tanya Sharma said:
Hi Chet...

Sorry for the late response .

Let h be the length of the normal ; x length of the left string and y length of the right string ; a and b be the length of the bases of left and right triangles respectively at t=0.

x=hcosecθ and y=hcosec30°
a=hsecθ and b=hsec30°

Now after time Δt ,

a' = a-3.25Δt
h' = h+Δt
b' = b+√3t

Now x+y = √(a'2+h'2) + √(b'2+h'2)

[tex]hcosecθ+hcosec30° = \sqrt{(hsecθ-3.25Δt)^2+(h+Δt)^2} + \sqrt{(hsec30°+\sqrt{3}Δt)^2+(h+Δt)^2}[/tex]

Is it correct ?
Ooops. Those sec's should be cots.

Chet
 
Tanya Sharma said:
If the pulley was not moving ,then we could have equated the component of velocities of the two blocks along the string .

But,since the pulley is moving,something extra needs to be done .Not sure what .

I would be grateful if somebody could help me with the problem .

You know the motion of everything. The blocks move horizontally, with the given velocities.
The pulley moves vertically upward with 1 m/s.

The string is tight, and it can move on the pulley. The total length is constant.

Choose the origin on the ground, just below the pulley. The positions of the blocks are A (xa,0) and B(xB,0). The pulley is at P(0,y). Write up the length of the pieces LA, LB. LA+ LB=constant. Take the derivative with respect to time. You know the derivative of dxA/dt=3.25, dXB/dt=√3, dy/dt=1. y/(-xA)=tanθ, y/xB=tan(30°)...


ehild
 
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Chestermiller said:
Ooops. Those sec's should be cots.

Chet

Yes...poor effort on my part :redface:.

If I open the expression under the radical sign ,I get lot of terms none of which seem to cancel.

Now what to do with terms containing Δt and Δt2 ?

Chestermiller said:
Expand each of the two hypotenuses as a linear function of Δt. Certain terms will cancel from both sides of the equation. Set the coefficient of Δt equal to zero.

Sorry...I didn't quite understand this .
 
  • #10
Tanya Sharma said:
Yes...poor effort on my part :redface:.

If I open the expression under the radical sign ,I get lot of terms none of which seem to cancel.

Now what to do with terms containing Δt and Δt2 ?



Sorry...I didn't quite understand this .
Discard the (Δt)2 terms.

[tex]\sqrt{(hcotθ-3.25Δt)^2+(h+Δt)^2}≈\sqrt{h^2(cot^2θ+1)+2hΔt(1-3.25cotθ)}≈hcscθ\sqrt{1+\frac{2hΔt(1-3.25cotθ)}{h^2csc^2θ}}[/tex]
[tex]\sqrt{(hcotθ-3.25Δt)^2+(h+Δt)^2}≈hcscθ+Δt(sinθ-3.25cosθ)[/tex]

Chet
 
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  • #11
Thanks ehild :smile:...Very nice and systematic way of looking at the problem.

But I seem to be struggling with sign errors :shy:. I don't get correct answer with the data you have given .Yet it looks fine to me.

ehild said:
Choose the origin on the ground, just below the pulley. The positions of the blocks are A (xa,0) and B(xB,0). The pulley is at P(0,y). Write up the length of the pieces LA, LB. LA+ LB=constant. Take the derivative with respect to time. You know the derivative of dxA/dt=3.25, dXB/dt=√3, dy/dt=1. y/(-xA)=tanθ, y/xB=tan(30°)...


ehild

If instead of treating (xa,0) and B(xB,0) as coordinates of A and B ,I look them as length (distance ) from the origin ,I get correct answer .

Then we would have

dxA/dt = -3.25, dXB/dt=√3, dy/dt=1. y/(xA)=tanθ, y/xB=tan(30°)

But I don't understand what is the problem with treating xa and xB as coordinates instead of lengths(distances).
 
Last edited:
  • #12
I can not know if you do not show your work...

ehild
 
  • #13
I like Pranav's approach to this problem. No calculus or expressions for the length of the string needed. In his frame of reference, the pulley has only rotational motion.
 
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  • #14
TSny said:
I like Pranav's approach to this problem. No calculus or expressions for the length of the string needed. In his frame of reference, the pulley has only rotational motion.

Yes, it is very nice...

ehild
 
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  • #15
This problem can be simplified by using Virtual-Work Method.
 
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  • #16
Please see this post in conjunction with my earlier post.

[tex]\sqrt{{x_A}^2+y^2} + \sqrt{{x_B}^2+y^2} = constant[/tex]

[tex]\frac{2x_A\frac{dx_A}{dt}+2y\frac{dy}{dt}}{2\sqrt{{x_A}^2+y^2}} + \frac{2x_B\frac{dx_B}{dt}+2y\frac{dy}{dt}}{2\sqrt{{x_B}^2+y^2}}[/tex]

[tex]\frac{\frac{dx_A}{dt}+\frac{y}{x_A}\frac{dy}{dt}}{\sqrt{1+{\frac{y}{x_A}}^2}} + \frac{\frac{dx_B}{dt}+\frac{y}{x_B}\frac{dy}{dt}}{\sqrt{1+{\frac{y}{x_B}}^2}}[/tex]

On putting in values given in post#8 we get

[tex]\frac{3.25-tanθ}{secθ} + 2 = 0[/tex] which gives incorrect result .

Whereas if I use values in post#11 I get [itex]\frac{-3.25+tanθ}{secθ} + 2 = 0[/itex] ,which gives correct result .

Could you reflect on this .
 
  • #17
Tanya Sharma said:
Please see this post in conjunction with my earlier post.

[tex]\sqrt{{x_A}^2+y^2} + \sqrt{{x_B}^2+y^2} = constant[/tex]

[tex]\frac{2x_A\frac{dx_A}{dt}+2y\frac{dy}{dt}}{2\sqrt{{x_A}^2+y^2}} + \frac{2x_B\frac{dx_B}{dt}+2y\frac{dy}{dt}}{2\sqrt{{x_B}^2+y^2}}[/tex]

[tex]\frac{\frac{dx_A}{dt}+\frac{y}{x_A}\frac{dy}{dt}}{\sqrt{1+{\frac{y}{x_A}}^2}} + \frac{\frac{dx_B}{dt}+\frac{y}{x_B}\frac{dy}{dt}}{\sqrt{1+{\frac{y}{x_B}}^2}}[/tex]

On putting in values given in post#8 we get

[tex]\frac{3.25-tanθ}{secθ} + 2 = 0[/tex] which gives incorrect result .

Whereas if I use values in post#11 I get [itex]\frac{-3.25+tanθ}{secθ} + 2 = 0[/itex] ,which gives correct result .

Could you reflect on this .

I think the problem lies in assuming the coordinate of left block as (x_a,0). It should be (-x_a,0) instead, where x_a>0. Now, if you closely look at [itex]d x_a /dt[/itex] which is the rate of change of x_a, you will find that it is -ve. This is because as the left block progresses towards the origin, x_a(which was initially some +ve quantity) approaches zero which clearly shows that x_a is decreasing and a -ve sign must be placed along with 3.25. Thus the second equation is the correct one.
 
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  • #18
utkarshakash said:
I think the problem lies in assuming the coordinate of left block as (x_a,0). It should be (-x_a,0) instead, where x_a>0. Now, if you closely look at [itex]d x_a /dt[/itex] which is the rate of change of x_a, you will find that it is -ve. This is because as the left block progresses towards the origin, x_a(which was initially some +ve quantity) approaches zero which clearly shows that x_a is decreasing and a -ve sign must be placed along with 3.25. Thus the second equation is the correct one.

Your reasoning looks quite convincing . Thanks :)
 
  • #19
You pulled out xA from the square root, which is negative. It should have been |xA|. ##\sqrt{(-2)^2}=2## and not -2.
I pulled out y and got correct result.

ehild
 
Last edited:
  • #20
ehild said:
You pulled out xA from the square root, which is negative. It should have been |xA|.
I pulled out y and got correct result.

ehild

Excellent troubleshooting !

If you had given me one whole day , i wouldn't have found that error :-p
 
  • #21
Tanya Sharma said:
Excellent troubleshooting !

If you had given me one whole day , i wouldn't have found that error :-p

It took me quite a long time, too. Now you will remember to to pull out only absolute value of something from the square root.:smile:

ehild
 

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