Difference between revisions of "Forest UCM NLM BlockOnInclineWfriction"

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: <math>\int_0^t  g \left ( \sin \theta - \mu \right ) dt = \int_0^v dv </math>
 
: <math>\int_0^t  g \left ( \sin \theta - \mu \right ) dt = \int_0^v dv </math>
  
 
+
: <math>v=\g \left ( \sin \theta - \mu \right ) t </math>
  
  
 
[[Forest_UCM_NLM#Block_on_incline_with_friction]]
 
[[Forest_UCM_NLM#Block_on_incline_with_friction]]

Revision as of 21:00, 20 August 2014

The problem

Consider a block of mass m sliding down the inclined plane shown below with a frictional force that is given by

[math]F_f = \mu mg[/math]


200 px

Find the blocks speed as a function of time.

Step 1: Identify the system

The block is the system with the following external forces, A normal force, a gravitational force, and the force of friction.

Step 2: Choose a suitable coordinate system

A coordinate system with one axis along the direction of motion may make solving the problem easier

Step 3: Draw the Free Body Diagram

200 px

Step 4: Define the Force vectors using the above coordinate system

[math]\vec{N} = \left | \vec{N} \right | \hat{j}[/math]
[math]\vec{F_g} = \left | \vec{F_g} \right | \left ( \sin \theta \hat{i} - \cos \theta \hat{j} \right )= mg \left ( \sin \theta \hat{i} - \cos \theta \hat{j} \right )[/math]
[math]\vec{F_f} = - \mu mg \hat{i}[/math]

Step 5: Used Newton's second law

in the [math]\hat i[/math] direction

[math]\sum F_{ext} = mg \sin \theta - \mu mg= ma_x = m \frac{dv_x}{dt}[/math]
[math]\int_0^t g \left ( \sin \theta - \mu \right ) dt = \int_0^v dv [/math]
[math]v=\g \left ( \sin \theta - \mu \right ) t [/math]


Forest_UCM_NLM#Block_on_incline_with_friction