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Grade 10Electric Current

in pull type 3 when the const eq comes out to be a1+a2+2a3=0 then i dont understant how one inextensible string has 2 accn because we know when 2 objects are coneccted with a string the have the same accn please refer illustarion 2 in the given article http://www.goiit.com/posts/show/813294/newtons-laws-of-motion-constraint-motion-804174.htm

Profile image of Hrishant Goswami
12 Years agoGrade 10
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1 Answer

Profile image of Askiitians Tutor Team
ApprovedApproved Tutor Answer11 Months ago

Let's break down the situation you're describing regarding the pull type 3 system and the equation \( a_1 + a_2 + 2a_3 = 0 \). It can indeed be a bit confusing at first, especially when considering the behavior of connected objects and the constraints imposed by the inextensible string. To clarify, we need to analyze the system step by step.

Understanding the System

In a typical scenario involving two objects connected by a string, you are correct that they share the same acceleration due to the inextensibility of the string. However, when we introduce additional constraints or components, such as pulleys or multiple segments of the string, the situation can change.

Breaking Down the Equation

The equation \( a_1 + a_2 + 2a_3 = 0 \) suggests that the accelerations of the three segments of the system are interrelated. Here’s how to interpret it:

  • a1: This is the acceleration of the first mass (let's call it mass 1).
  • a2: This is the acceleration of the second mass (mass 2).
  • a3: This represents the acceleration of a segment of the string or another mass in the system.

Why Two Accelerations?

In this particular case, the presence of the term \( 2a_3 \) indicates that the acceleration of the string segment (or the third mass) is affecting the overall motion of the system. This can happen in scenarios where:

  • The string is looped around a pulley, creating a situation where the motion of one segment influences the others.
  • There are additional forces acting on the system that cause different accelerations for the connected masses.

Illustrating with an Example

Imagine a scenario where you have two blocks connected by a string over a pulley. If you pull down on one side of the string, both blocks will accelerate, but if the pulley is not frictionless or if there are additional weights or forces acting on one of the blocks, the accelerations can differ. For instance:

  • If mass 1 is hanging and mass 2 is on a frictionless surface, pulling down on mass 1 will cause it to accelerate downward while mass 2 accelerates horizontally.
  • If the string has a segment that is also accelerating (like a third mass attached to the string), this can lead to the equation you provided, where the accelerations are not simply equal but rather depend on the configuration of the entire system.

Visualizing the Motion

To visualize this, think of a seesaw. If one side goes down, the other side goes up, but if you add weights or change the pivot point, the motion becomes more complex. Similarly, in your system, the accelerations are linked through the constraints of the string, leading to the equation that combines them in a specific way.

Final Thoughts

In summary, while it’s true that connected objects typically share the same acceleration, the presence of additional constraints or configurations can lead to different accelerations for each segment of the system. The equation \( a_1 + a_2 + 2a_3 = 0 \) reflects this complexity, capturing the interplay between the different accelerations. By carefully analyzing the forces and constraints at play, you can gain a clearer understanding of how these systems operate.