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A block of mass m1=3.70kgon a frictionless plane inclined at angle θ=30.00is connected by a cord over a massless, frictionless pulley to a second block of massm2=2.30kg(Figure). (a) What is the magnitude of the acceleration of each block, (b) What is the direction of the acceleration of the hanging block, and (c) What is the tension in the cord?

Short Answer

Expert verified

(a) Magnitude of acceleration of each block is0.735m/s2

(b) Direction of the acceleration of the hanging block is down-ward.

(c) The tension in the cord is 20.8N

Step by step solution

01

Given information

  1. m1=3.70kg
  2. m2=2.30kg

3.θ=30.0°

02

Understanding the concept of Newton’s law

From Newton’s second law, the net force on the body is equal to the vector sum of all the forces acting. The force is equal to the product of the mass of the body and its acceleration.

Apply Newton’s second law to each block to get the acceleration.

Formula:

F = ma (i)

Here, F is the net force, m is the mass of the body, and a is acceleration.

03

(a) Calculate the magnitude of the acceleration of each block

The equation of motion for block 1 along the inclined plane is

T-m1gsinθ=m1a

Rearranging this equation for tension T, we get

T=m1gsinθ+m1a (ii)

And the equation of motion for block 2 is

T-m2g=-m2a

Rearranging this equation for tension T, we get

T=m2g-m2a (iii)

Solving equations (ii) and (iii), we get

a=m2g-m1gsinθm1+m2

Substitute the values in the above equation to calculate acceleration.

a=2.30kg-3.70kg.30°9.8m/s23.70kg+2.30kg=0.735m/s2

Therefore, the acceleration is0.735m/s2 .

04

(b) Calculate the direction of the acceleration of the hanging block

As the value of acceleration is positive, the direction of acceleration is in line with equations of motion. So, the direction of acceleration of the hanging block is downward.

05

(c) Calculate the tension in the cord

We can calculate the tension using either equation (iii), we get

T=m2g-m2a=2.30kg×9.8m/s2-3.70kg×0.735m/s2=20.8N

Therefore, the tension in the cord is20.8N .

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