plan for today (ap physics 2)

27

Upload: xanthe

Post on 22-Feb-2016

30 views

Category:

Documents


0 download

DESCRIPTION

Plan for Today (AP Physics 2). Turn in lab from yesterday C Test Takers: Go over MC Notes/Lecture Variable Forces Drag Equation Derivation B Test Takers: MOPing on computers ( pick a problem area). Calculating Work a Different Way. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Plan for Today (AP Physics 2)
Page 2: Plan for Today (AP Physics 2)
Page 3: Plan for Today (AP Physics 2)

Plan for Today (AP Physics 2)• Turn in lab from yesterday• C Test Takers:

• Go over MC• Notes/Lecture Variable Forces• Drag Equation Derivation

• B Test Takers:• MOPing on computers (pick a problem area)

Page 4: Plan for Today (AP Physics 2)

Calculating Work a Different Way• Work is a scalar resulting from the multiplication of two vectors.• We say work is the “dot product” of force and displacement.• W = F • r

• dot product representation

• W= F r cos q• useful if given magnitudes and directions of vectors

• W = Fxrx + Fyry + Fzrz• useful if given unit vectors

Page 5: Plan for Today (AP Physics 2)

The “scalar product” of two vectors is called the “dot product”• The “dot product” is one way to multiply two vectors. (The other way

is called the “cross product”.)• Applications of the dot product

• Work W = F d• Power P = F v• Magnetic Flux ΦB = B A

• The quantities shown above are biggest when the vectors are completely aligned and there is a zero angle between them.

Page 6: Plan for Today (AP Physics 2)

Why is work a dot product?

s

W = F • rW = F r cos qOnly the component of force aligned with displacement does work.

Fq

Page 7: Plan for Today (AP Physics 2)

Work and Variable Forces• For constant forces

• W = F • r• For variable forces, you can’t move far until the force changes.

The force is only constant over an infinitesimal displacement.• dW = F • dr

• To calculate work for a larger displacement, you have to take an integral

• W = dW = F • dr

Page 8: Plan for Today (AP Physics 2)

Variable Forces• If force can vary, what should our new equation for work look like?

• W =

• This would be by a position dependent force

Page 9: Plan for Today (AP Physics 2)

Work and variable forceThe area under the curve of a graph of force vs displacement gives the work done by the force.

F(x)

xxa xb

W = F(x) dxxa

xb

Page 10: Plan for Today (AP Physics 2)

What if force varies with time? • F = ma• a = dv/dt• a = • F = m = mv

• = dx• = dx =

Page 11: Plan for Today (AP Physics 2)

Let’s Integrate that• = dx =

• = • = • =

• Look familiar?• It’s the Work-Energy theorem• Work is equal to the change in kinetic energy• And it holds constant whether a force is constant or not

Page 12: Plan for Today (AP Physics 2)

What if it’s potential energy• Force of a spring• = - kx• Hooke’s Law• = = • =• ½ k

Page 13: Plan for Today (AP Physics 2)

Spring Potential Energy, Us

• Springs obey Hooke’s Law.• Fs(x) = -kx

• Fs is restoring force exerted BY the spring.

• Ws = Fs(x)dx = -k xdx• Ws is the work done BY the spring.

• Us = ½ k x2

• Unlike gravitational potential energy, we know where the zero potential energy point is for a spring.

Page 14: Plan for Today (AP Physics 2)

Conservative Forces and Potential Energy• = = Change in potential energy• + Ui

• dU = - dx

• = - dU/dx

Page 15: Plan for Today (AP Physics 2)

Force and Potential Energy• In order to discuss the relationships between potential energy and

force, we need to review a couple of relationships.• Wc = FDx (if force is constant)

• Wc = Fdx = - dU = -DU (if force varies)

• Fdx = - dU• Fdx = -dU• F = -dU/dx

Page 16: Plan for Today (AP Physics 2)

Power• P = dE/dt• Average Power = W/t

• P = dW/dt = F * dr/dt = F * v

Page 17: Plan for Today (AP Physics 2)

Forces Reminders• Be sure to draw freebody diagrams• Think about net force and what is going on there

Page 18: Plan for Today (AP Physics 2)

Drag and Resistive forces• Drag is a resistive force proportional to the object’s velocity• How can we express this?

• = -bv• v is velocity• b is a constant

• Depends on the properties of the medium, shape of the object, size of the object

Page 19: Plan for Today (AP Physics 2)

Considering Drag with other forces• Think about the coffee filter lab. • What forces were acting on the coffee filter?

• = mg – bv = ma

Page 20: Plan for Today (AP Physics 2)

Eventually, the coffee filters reached terminal velocity

Page 21: Plan for Today (AP Physics 2)
Page 22: Plan for Today (AP Physics 2)

How can we figure out the terminal velocity? • mg - b = 0• =

Page 23: Plan for Today (AP Physics 2)

How can we figure out the velocity at any given point? • mg – bv = ma

• a = • = g -

Page 24: Plan for Today (AP Physics 2)

Assignment• Solve the equation to get an expression for v for all times t (no ds in

there)

• = g -

Page 25: Plan for Today (AP Physics 2)

• Sample problem: Gravitational potential energy for a body a large distance r from the center of the earth is defined as shown below. Derive this equation from the Universal Law of Gravity.

1 2g

GmmUr

• Hint 1: dW = F(r)•dr• Hint 2: ΔU = -Wc (and gravity is conservative!)• Hint 3: Ug is zero at infinite separation of the masses.

Page 26: Plan for Today (AP Physics 2)

• Problem: The potential energy of a two-particle system separated by a distance r is given by U(r) = A/r, where A is a constant. Find the radial force F that each particle exerts on the other.

Page 27: Plan for Today (AP Physics 2)

• Problem: A potential energy function for a two-dimensional force is of the form U = 3x3y – 7x. Find the force acting at a point (x,y).