stephysics.blogspot.com

STEP Physics

Sunday, April 1, 2012. Its due April 28. Use any tools at your disposal. Don't forget your name. If you're going to be absent email me the answers. Tuesday, February 21, 2012. Put simply, momentum is mass in movement and is described by p= mv. P=momentum, m=mass, v=velocity). One of the great things is that momentum is conserved (well conserved in perfect situations, but we'll talk more about that later). Sunday, February 12, 2012. More on balancing forces and force diagrams. Subscribe to: Posts (Atom).

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STEP Physics | stephysics.blogspot.com Reviews

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Sunday, April 1, 2012. Its due April 28. Use any tools at your disposal. Don't forget your name. If you're going to be absent email me the answers. Tuesday, February 21, 2012. Put simply, momentum is mass in movement and is described by p= mv. P=momentum, m=mass, v=velocity). One of the great things is that momentum is conserved (well conserved in perfect situations, but we'll talk more about that later). Sunday, February 12, 2012. More on balancing forces and force diagrams. Subscribe to: Posts (Atom).

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STEP Physics | stephysics.blogspot.com Reviews

https://stephysics.blogspot.com

Sunday, April 1, 2012. Its due April 28. Use any tools at your disposal. Don't forget your name. If you're going to be absent email me the answers. Tuesday, February 21, 2012. Put simply, momentum is mass in movement and is described by p= mv. P=momentum, m=mass, v=velocity). One of the great things is that momentum is conserved (well conserved in perfect situations, but we'll talk more about that later). Sunday, February 12, 2012. More on balancing forces and force diagrams. Subscribe to: Posts (Atom).

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stephysics.blogspot.com

1

STEP Physics: More on balancing forces and force diagrams.

http://stephysics.blogspot.com/2012/02/more-on-balancing-forces-and-force.html

Sunday, February 12, 2012. More on balancing forces and force diagrams. For bodies connected by a cable. ( the * in part d should be an x, representing the x-axis.). Subscribe to: Post Comments (Atom). More on balancing forces and force diagrams. Notes 2/11/2012: Balancing Forces. Notes 2/4/2012: Applications of Newtons Laws. Simple template. Powered by Blogger.

2

STEP Physics: December 2011

http://stephysics.blogspot.com/2011_12_01_archive.html

Sunday, December 18, 2011. Here is the link for Exam 2. For those of you who lost it or weren't here on 12/17. You are encouraged to use any/all resources all your disposal. Just like before, the exam is due the date you come back from the break, 1/21/12. Saturday, December 17, 2011. Topic Today: Projectile Motion. The biggest challenge behind these problems is:. 1 Projecting your initial velocity (at an angle) into your x and y projections. Your x and y dimension vectors are INDEPENDENT. Time. This week...

3

STEP Physics: November 2011

http://stephysics.blogspot.com/2011_11_01_archive.html

Sunday, November 20, 2011. Today was the culminating lesson of kinematics.the use of formulas in representing motion. It is also one of the most difficult topics to fully master because it involves math. I've updated my notes on Kinematics. With the latest information on what we did in class. Please read if you have not already done so. At the end of class some of your classmates posted solutions to the worksheet. Once again, use the Physics Classroom. Saturday, November 19, 2011. If you think you might.

4

STEP Physics: Exam 3

http://stephysics.blogspot.com/2012/04/heres-exam-3-its-due-april-28.html

Sunday, April 1, 2012. Its due April 28. Use any tools at your disposal. Don't forget your name. If you're going to be absent email me the answers. Subscribe to: Post Comments (Atom). Simple template. Powered by Blogger.

5

STEP Physics: February 2012

http://stephysics.blogspot.com/2012_02_01_archive.html

Tuesday, February 21, 2012. Put simply, momentum is mass in movement and is described by p= mv. P=momentum, m=mass, v=velocity). One of the great things is that momentum is conserved (well conserved in perfect situations, but we'll talk more about that later). Sunday, February 12, 2012. More on balancing forces and force diagrams. For bodies connected by a cable. ( the * in part d should be an x, representing the x-axis.). Subscribe to: Posts (Atom). More on balancing forces and force diagrams.

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Sunday, April 1, 2012. Its due April 28. Use any tools at your disposal. Don't forget your name. If you're going to be absent email me the answers. Tuesday, February 21, 2012. Put simply, momentum is mass in movement and is described by p= mv. P=momentum, m=mass, v=velocity). One of the great things is that momentum is conserved (well conserved in perfect situations, but we'll talk more about that later). Sunday, February 12, 2012. More on balancing forces and force diagrams. Subscribe to: Posts (Atom).

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