plan for today (ap physics 2)
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 PresentationTRANSCRIPT
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• 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
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.
Why is work a dot product?
s
W = F • rW = F r cos qOnly the component of force aligned with displacement does work.
Fq
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
Variable Forces• If force can vary, what should our new equation for work look like?
• W =
• This would be by a position dependent force
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
What if force varies with time? • F = ma• a = dv/dt• a = • F = m = mv
• = dx• = dx =
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
What if it’s potential energy• Force of a spring• = - kx• Hooke’s Law• = = • =• ½ k
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.
Conservative Forces and Potential Energy• = = Change in potential energy• + Ui
• dU = - dx
• = - dU/dx
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
Power• P = dE/dt• Average Power = W/t
• P = dW/dt = F * dr/dt = F * v
Forces Reminders• Be sure to draw freebody diagrams• Think about net force and what is going on there
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
Considering Drag with other forces• Think about the coffee filter lab. • What forces were acting on the coffee filter?
• = mg – bv = ma
Eventually, the coffee filters reached terminal velocity
How can we figure out the terminal velocity? • mg - b = 0• =
How can we figure out the velocity at any given point? • mg – bv = ma
• a = • = g -
Assignment• Solve the equation to get an expression for v for all times t (no ds in
there)
• = g -
• 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.
• 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.
• 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).