Flag Mechanics> string-pulley-constraints...
question mark

I just don't get it. I've tried every method- 1) making the length of the string constant and differentiating to get relation between accelerations,2) imagining what would happen if pulley moves a distance x,also 3) aT=a'T'.I can apply the first two in simple problems but as the problems become more complex I find them difficult to apply.The latter is not applicable in all situations. I've tried every video there is on the internet explaining this concept but all the examples they give are way too easy.Please help me.Also,take a difficult example while explaining

Kunjal Shah , 12 Years ago
Grade
anser 1 Answers
Askiitians Tutor Team

It sounds like you're grappling with the complexities of dynamics, particularly in systems involving pulleys and strings. This can indeed be challenging, especially as problems become more intricate. Let's break this down step by step, using a more complex example to clarify the concepts you're struggling with.

Understanding the Dynamics of a Pulley System

Consider a scenario where we have a pulley system with two masses, \( m_1 \) and \( m_2 \), connected by a string over a frictionless pulley. Let's say \( m_1 = 5 \, \text{kg} \) is hanging vertically, and \( m_2 = 3 \, \text{kg} \) is on a horizontal surface with friction. The coefficient of friction between \( m_2 \) and the surface is \( \mu = 0.2 \). We want to find the acceleration of the system when released from rest.

Step 1: Identify Forces Acting on Each Mass

For \( m_1 \), the forces acting on it are:

  • The gravitational force downward: \( F_{g1} = m_1 \cdot g = 5 \cdot 9.81 = 49.05 \, \text{N} \)
  • The tension in the string upward: \( T \)

For \( m_2 \), the forces are:

  • The tension in the string pulling it horizontally: \( T \)
  • The frictional force opposing the motion: \( F_{friction} = \mu \cdot m_2 \cdot g = 0.2 \cdot 3 \cdot 9.81 = 5.886 \, \text{N} \)

Step 2: Set Up the Equations of Motion

Now, we can write the equations of motion for both masses. For \( m_1 \):

Using Newton's second law, we have:

\( m_1 \cdot a = m_1 \cdot g - T \)

Substituting the values:

\( 5a = 49.05 - T \) (1)

For \( m_2 \):

\( m_2 \cdot a = T - F_{friction} \)

Substituting the values:

\( 3a = T - 5.886 \) (2)

Step 3: Solve the System of Equations

Now we have two equations (1) and (2) with two unknowns, \( T \) and \( a \). We can express \( T \) from equation (1):

\( T = 49.05 - 5a \)

Substituting this expression for \( T \) into equation (2):

\( 3a = (49.05 - 5a) - 5.886 \)

Combine like terms:

\( 3a + 5a = 49.05 - 5.886 \)

\( 8a = 43.164 \)

Now, solving for \( a \):

\( a = \frac{43.164}{8} \approx 5.3955 \, \text{m/s}^2 \)

Step 4: Find the Tension in the String

Now that we have the acceleration, we can substitute \( a \) back into one of our equations to find the tension:

Using \( T = 49.05 - 5a \):

\( T = 49.05 - 5 \cdot 5.3955 \)

\( T \approx 49.05 - 26.9775 \approx 22.0725 \, \text{N} \)

Key Takeaways

In this example, we tackled a more complex pulley system involving friction. The key steps involved:

  • Identifying all forces acting on each mass.
  • Setting up equations of motion using Newton's second law.
  • Solving the system of equations to find the unknowns.

When dealing with more complicated problems, remember to break them down into manageable parts, just like we did here. Each mass has its own forces and equations, and by systematically solving them, you can find the relationships between acceleration, tension, and other variables. Practice with different scenarios, and over time, you'll find these concepts becoming clearer and more intuitive.

ApprovedApproved
Last Activity: 8 Months ago
star
LIVE ONLINE CLASSES

Prepraring for the competition made easy just by live online class.

tv

Full Live Access

material

Study Material

removal

Live Doubts Solving

assignment

Daily Class Assignments