Other Physics Flashcards
Torque
Measure of a force’s ability to cause rotational acceleration
If force acts at any point on an object other than the center of mass, object accelerates rotationally
/tau = F r sin\theta
Torque is a vector (can be clockwise or counter-clockwise)
Where r is position of force application to the point of rotation
When l is lever arm, force is applied perpendicularly to r and sin \theta = 1
Greater the net torque on an object, greater the acceleration
Work
W = Fd
In units of Joules = Newton meters
Useful simplification of thermodynamic equations for MCAT when no friction:
W + q = \delta K + \delta U
What are the ways energy can be divided?
Energy can be divided into mechanical and non-mechanical energies Mechanical energy (\delta Em): energy of a macroscopic system - Potential energy: energy of position - Kinetic energy: K = 1/2 mv^2, energy of motion
Power
Rate of energy transfer
P = W/t = \delta E / t = Fd cos \theta / t = Fv cos \theta (theta is angle between F and v)
Law of Conservation of Mechanical Energy
When only conservative forces are acting, the sum of mechanical energies remains constant
K1 + U1 = K2 + U2 (conservative forces only, no heat)
Conservative force: if mechanical energy prior equals mechanical energy after, conservative force, force must be a function of position only
What are some example of conservative vs. non-conservative forces?
Conservative forces: gravitational energy, elastic potential energy of a spring
Non-conservative forces: kinetic frictional forces, pushing and pulling forces of humans or animals, sum of potential and kinetic energies remains constant
Except for frictional forces, work done by all non-conservative forces = change in mechanical energy of systems upon which they are applied
W = \delta K + \delta U
Technically speaking, a conservative force does not do work bc energy is never gained or lost by the system
Mechanical advantage
The ability to reduce applied force required to do a given amount of work
- Machines are able to reduce force, but do not change work
Ramp
Inclined plane that reduces force needed to do work by increasing distance over which force is applied (think about W = Fd)
Force needed is only mg sin\theta instead of mg to lift an object to top of ramp (by sliding on ramp instead)
E.g. to reduce the force to 1/2 mg, make a ramp that is 2h long
Length of ramp calculated by: h/sin \theta
We can see that work, W = mg sin\theta x h / sin \theta = mgh, and did not change
Lever
Beam attached to fulcrum (pivot point)
Reduces force needed to do a given amount of work by increasing distance over which the force is applied (similar to ramp)
- Based on principle of torque, and remember work is always the same
- Doubling the length of the lever arm reduces the force required by a factor of two
Torque = F x L
If lifting mass, then balance the torques of two ends of the lever:
- torque1 = mg x L1, torque2 = F x L2
- F = mg L1 / L2
Pulley
Allows force to act over a greater distance so that the same amount of work can be done with less force
- Uses rope to increase distance over which the force acts
- Magnitude of force acting throughout the length of rope is called tension
- Tension is scalar and has no direction, assume that tension throughout a rope is constant (same at every point), means ideal pulley
Specific Gravity
Symbol SG = \ro_substance / \ro_water
Specific gravity less than 1 indicates substance lighter than water
\ro_water = 1000 kg/m^3 = 1 g/cm^3
Fluid pressure
Pressure experienced by object as a result of impulse of molecular collisions
It is average of magnitudes of change in momentum of collisions divided by time duration of collisions
P = F / A = \ro g y (for fluid at rest with uniform density in sealed container)
SI unit is Pascal, a scalar quantity
Fluid at rest experiences only forces perpendicular to surface
How can the total pressure of a column of different fluids be found?
Adding the pressures due to each fluid:
Ptotal = \ro_1 g y_1 + \ro_2 g y_2 + \ro_3 g y_3 + …
Must add atmospheric pressure if the container is open to the air as well
In any fluid open to atmosphere:
P = \ro g y + Patm
At sea level, Patm = 101,000 Pa = 1 atm
Pascal’s principle
Pressure applied anywhere to an enclosed incompressible fluid will be distributed undiminished through teh fluid
Gauge Pressure
Amount by which a system’s pressure deviates from atmospheric pressure
Pabs = Pgauge + Patm
Absolute pressure: pressure of a system relative to a vacuum
Hydraulic Lift
Simple machine that works via Pascal’s principle
Two pistons and a container enclose a standing incompressible fluid
Force applied on piston with less area, which gets transferred undiminished to piston 2 which has greater area, therefore translating to greater force (does not change work)
Distance compressed at piston 1 is greater than distance travelled at piston 2
Buoyant force
Standing fluid exerts this force on any object that is floating, submerged, or sunk in the fluid
Both pressure and force increase with depth, causing an object in fluid to experience both greater pressure and greater force at points farther from fluid’s surface (object experiences upward force)
The difference in pressure (and therefore force) experienced by points closest to and farthest from the water surface (on the same object) creates upward buoyant force
Since the lower surface of a fully submerged box experiences greater pressure on the surface than the upper surface of a fully submerged box, it experiences a net upward force
Archimede’s Principle
F_B = \ro_fluid V_fluid g = (m_fluid / V_fluid)(V_fluid) g = m_fluid g, V_fluid is volume of fluid displaced
Upward buoyant force is equal in magnitude to weight of displaced fluid
How do you compute the fraction of an object that will be submerged in water?
Fraction submerged = \ro_object / \ro_fluid = V_fluid / V_object
Floating object:
F_B = \ro_fluid V_fluid g = m_fluid g = F_G = m_object g
Simplifies to m_fluid = m_object because floating object displaces a volume of fluid with a mass equal to its own mass
Object only floats when density is less than density of fluid on which it floats
Case of submerged object
If upward buoyant force equals downward force of gravity when \delta y are their maximum values, object is submerged
Submerged object is like a floating object that does not sink, but entirety of submerged object is within the fluid
m_fluid = m_object, V_fluid = V_object
\ro_fluid must equal \ro_object
F_B = \ro_fluid V_fluid g, F_g,object = \ro_object V_object g
Case of the sunk object
Sunk object displaces a volume of fluid equal to its own volume and experiences upward buoyant force that is less than downward gravitational force
Experiences net downward force that causes object to accelerate downward until it contacts a surface able to provide enough upward normal force to counter downward force of gravity
F_B < F_G, m_fluid < m_object, but V_fluid = V_object
F_B + F_N = F_G = m_object g, apparent weight is equal to difference between downward force of gravity and upward buoyant force
What is the apparent weight loss of an object?
\ro_fluid / \ro_object = m_fluid / m_object since volumes are equal
\ro_fluid / \ro_object x 100% = apparent weight loss of object
Center of buoyancy
Buoyant force acts at an object’s center of buoyancy, which is the point where the center of mass would be if the object had uniform density
If object is not uniformly dense, center of mass and center of buoyancy are not at the same place (resulting in torque)
What are the two types of fluid motion?
Random translational motion: contributes to fluid pressure as in a fluid at rest
Uniform translational motion: shared equally by all molecules at given location in fluid, does not contribute to fluid pressure
Some of random translational motion can be converted to uniform translational motion and vice versa