Acceleration of Block B in a Constrained Motion Problem

In summary, in this conversation, the acceleration of block B in a given figure is calculated assuming all surfaces and pulleys are smooth and light. The lengths of the strings and their derivatives are used to create equations and solve for the acceleration of each block. The equations for block A, B, and C are solved to get the final answer of \ddot{x_B}=\frac{3F}{13m}.
  • #1
Saitama
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Homework Statement


Calculate the acceleration of the block B in the figure, assuming the surfaces and the pulleys ##P_1## and ##P_2## are all smooth and pulleys and string are light.

(The mass of block C is m)

Ans: F/(7m)

Homework Equations





The Attempt at a Solution


I measured distances from a fixed wall on the right of B. The distances are shown in the second attachment.
Writing down the expression for length of string, (##R## is the radius of pulleys)
$$L=x_{P1}-x_B+\pi R+x_{P1}-x_{P2}+\pi R+x_{C}-x_{P2}$$
Differentiating twice with respect to time,
$$0=2\ddot{x_{P1}}-\ddot{x_B}-2\ddot{x_{P2}}+\ddot{x_{C}}$$
##\because \ddot{x_{P1}}=\ddot{x_A}## and ##\ddot{x_{P2}}=\ddot{x_{B}}##
$$2\ddot{x_A}=3\ddot{x_B}-\ddot{x_C} (*)$$
Assume that the tension in the string is T. Applying Newton's second law for A,
$$F-2T=2m\ddot{x_A} (**)$$
For B,
$$3T=4m\ddot{x_B} (***)$$
For C,
$$T=m\ddot{x_C} (****)$$
Solving the four equations,
[tex]\ddot{x_B}=\frac{3F}{13m}[/tex]

Any help is appreciated. Thanks!
 

Attachments

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  • #2
I would suggest to keep things simple.

Let the lengths be x1(top),x2(middle),x3(bottom).

A and B move to the left,C move to the right.

We have, [itex] \ddot{x_1}+\ddot{x_2}+\ddot{x_3}=0 [/itex]

[itex] \ddot{x_1}=a_A-a_B[/itex]

[itex]\ddot{x_2}=a_A-a_B[/itex]

[itex]\ddot{x_3}=-a_B-a_C[/itex]

where aA,aB,aC are magnitude of accelerations of blocks A,B,C.

aA = (F-2T)/(2m)

aB = 3T/(4m)

aC= T/m
 
  • #3
Tanya Sharma said:
I would suggest to keep things simple.

Let the lengths be x1(top),x2(middle),x3(bottom).

A and B move to the left,C move to the right.

We have, [itex] \ddot{x_1}+\ddot{x_2}+\ddot{x_3}=0 [/itex]

[itex] \ddot{x_1}=a_A-a_B[/itex]

[itex]\ddot{x_2}=a_A-a_B[/itex]

[itex]\ddot{x_3}=-a_B-a_C[/itex]

where aA,aB,aC are magnitude of accelerations of blocks A,B,C.

aA = (F-2T)/(2m)

aB = 3T/(4m)

aC= T/m

That does gives the answer but how do you get the second derivatives of lengths in terms of ##a_A##, ##a_B## and ##a_C##?
Using your method, I get ##2a_A=3a_B+a_C## where as from my method, I get ##2a_A=3a_B-a_C##. Where did I go wrong? :confused:
 
  • #4
Pranav-Arora said:
That does gives the answer but how do you get the second derivatives of lengths in terms of ##a_A##, ##a_B## and ##a_C##?

Lets consider case of x1:

What causes a change in x1?

Block A moving to the left causes x1 to increase and B moving to the left causes the string length x1 to decrease.So, [itex]\dot{x_1}={v_A}-{v_B}[/itex],where [itex]{v_A}[/itex] and[itex] {v_B}[/itex] are speeds of a and B respectively.

Hence [itex]\ddot{x_1}=\ddot{a_A}-\ddot{a_B}[/itex].
 
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  • #5
Tanya Sharma said:
Lets consider case of x1:

What causes a change in x1?

Block A moving to the left causes x1 to increase and B moving to the left causes the string length x1 to decrease.So, [itex]\dot{x_1}={v_A}-{v_B}[/itex],where [itex]{v_A}[/itex] and[itex] {v_B}[/itex] are speeds of a and B respectively.

Hence [itex]\ddot{x_1}=a_A-a_B[/itex].

Thanks! :)

Any idea what's wrong with my method?
 
  • #6
Pranav-Arora said:
For C,
$$T=m\ddot{x_C} (****)$$

It should be $$-T=m\ddot{x_C} (****)$$

You are considering left direction to be positive .:smile:
 
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  • #7
Tanya Sharma said:
It should be $$-T=m\ddot{x_C} (****)$$

You are considering left direction to be positive .:smile:

Great! Thanks a lot Tanya! :)
 

What is a constrained motion problem?

A constrained motion problem is a type of problem in physics that involves the motion of an object or system that is subject to certain constraints or restrictions. These constraints could include forces, boundaries, or other limitations that affect the motion of the object/system.

What are some common examples of constrained motion problems?

Examples of constrained motion problems include objects moving along a curved path, systems with fixed joints or hinges, and objects moving on a surface with friction. Other examples could include pendulums, pulley systems, and objects sliding on an inclined plane.

How do you solve a constrained motion problem?

To solve a constrained motion problem, you must first identify the constraints that are affecting the motion of the object or system. Then, you can use principles of physics, such as Newton's laws of motion and conservation of energy, to analyze the motion and find a solution. It may also be helpful to draw free body diagrams and use mathematical equations to solve for unknown variables.

What challenges are associated with solving constrained motion problems?

One challenge of solving constrained motion problems is determining the correct constraints to consider. In some cases, there may be multiple constraints that affect the motion, making the problem more complex. Additionally, the presence of friction or other non-ideal conditions can make the problem more difficult to solve.

Why are constrained motion problems important in science?

Constrained motion problems are important in science because they allow us to understand and predict the behavior of objects and systems in real-world situations. They also help us to develop and refine our understanding of physical laws and principles, and can be used to design and improve technologies and systems in various fields such as engineering, robotics, and biomechanics.

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