Difference between revisions of "Forest UCM NLM BlockOnIncline"
		
		
		
		
		
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| Line 23: | Line 23: | ||
:<math>\vec{N} = \left | \vec{N} \right | \hat{j}</math>  | :<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 )</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} = - kmv^2 \hat{i}</math>  | :<math>\vec{F_f} = - kmv^2 \hat{i}</math>  | ||
Revision as of 02:41, 19 August 2014
Consider a block of mass m sliding down the inclined plane shown below with a frictional force that is given by
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
Step 4: Define the Force vectors using the above coordinate system
Step 5: Used Newton's second law