AP Physics 1
First Semester Review of EVERYTHING I learned J
KINEMATICS:
· The general relationship between position, velocity, and acceleration:
o I can analyze x vs. t, v vs. t, and a vs. t graphs. I know the significance of the slope.
· I know 4 main kinematics equations:
· A vector is:
o The rules for adding and subtracting vectors:
o I know how to find a resultant vector using Pythagorean Theorem or trig to find either a side or an angle:
· I know how to use my 4 kinematics equations to solve problems in 2 dimensions:
o My 3 main “projectile” formulas:
o Velocity and acceleration in x-direction vs. y-direction:
o Steps for solving projectiles questions with an initial velocity:
o Basic picture of a projectile with velocity and acceleration vectors:
DYNAMICS/NEWTON’S LAWS
· Newton’s Three Laws:
o 1st –
o 2nd –
o 3rd –
· Net force means:
· If there is NO NET FORCE on an object, then the object is doing 1 of 2 things:
o The object is
o Or the object is
· I can draw a well-labeled free body diagram, for example:
· I know the steps for solving force problems…
o Hanging stop light questions:
o Pulley (Atwood) questions:
o Pulley on Table questions:
o Pulley on Ramp questions:
· When I sum my forces, I know that I can set them equal to 1 of 2 things:
o =
o =
· Friction is:
o I know about 2 types of friction and when each apply:
o What the coefficient of friction means:
o Formula for Frictional Force:
o I can figure out when an object will start to slip, for example:
· Terminal Velocity is:
o I can calculate terminal velocity, for example:
· Action-Reaction Pairs are:
· A great picture for remembering equal and opposite forces is:
WORK, ENERGY & POWER
· Work is:
o Work is positive when:
o Work is negative when:
o Work is zero when:
o 2 Formulas for Work:
· I can calculate work from a graph, for example:
· Work-Energy Theorem is represented by this equation:
o Example problem:
o I know that I have to find the ______on an object before finding the NET WORK done on an object.
o If I want to find the work done by a specific force, I use the component of that force in the direction of movement and work equation.
§ Example:
o I can figure out the stopping distance needed for an object using the Work-Energy Theorem.
§ Example:
o If an object is moving at a CONSTANT VELOCITY, then the NET WORK is ______.
§ BUT, work is still done on the object by the individual forces, for example:
· More formulas for this chapter:
o Work
o Kinetic Energy
o Gravitational Potential Energy
o Elastic Potential Energy
o Hooke’s Law
· Law of Conservation of Energy:
o I can use conservation of energy to solve problems in situations such as:
§ Atwood’s machine (simple pulley)
§ Pendulums (including ballistic pendulum)
§ Hanging Mass-Spring systems
§ Objects that slide and compress springs
§ Objects that change heights
· Power is:
o 4 Formulas for power:
o When a person is lifting themselves up (as in going up a flight of stairs), the force I use in the power equation is ______.
o When calculating the power needed to lift something up, the force I use in the power equation is______.
o When I calculate AVERAGE POWER, then I need to use AVERAGE VELOCITY.
LINEAR MOMENTUM
· Formulas:
o Momentum:
o Impulse:
o Impulse-Momentum Theorem:
o Conservation of Momentum:
· I can use graphs to solve momentum questions, for example:
o 1 type of collision in which the objects return to their original shape is:______
§ After colliding, the objects ______
§ Momentum is ______(conserved or not conserved?)
§ Kinetic Energy is ______
o Another type of collision where the objects deform or where significant heat is created is ______
§ After colliding, the objects can either ______or ______. If the objects have identical velocities after the collision, it is said to be a ______collision.
§ Momentum is ______
§ Kinetic Energy is ______
· I can find the loss of energy in a collision by:
· Impulse is equal to D______or F______. Airbags work by increasing ______and thus reducing ______on the occupant. An airbag (does, does not?) reduce impulse.
· Sample problem for 2 cars colliding in one and two dimensions.
· Sample problem for the change in momentum of an object produced by a force on that object exerted over a period of time.