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Label Description LG Status Operations
MassConserved (Copy) Mass is conserved. 0 Draft Edit
MaxwellEqn There are four Maxwell equations. 0 Draft Edit
MaxwellEqn (Copy) There are four Maxwell equations. 0 Draft Edit
MaxwellEqn (Copy) There are four Maxwell equations. 0 Draft Edit
MaxwellEqn (Copy) (Copy) There are four Maxwell equations. 0 Draft Edit
Mechanics Mechanics is the branch of classical physics that studies the motion of objects and the forces that cause or change that motion. 0 Draft Edit
Mechanics (Copy) Mechanics is the branch of classical physics that studies the motion of objects and the forces that cause or change that motion. 0 Draft Edit
Medium A medium is a material that light or other form of energy travels in or through. 0 Ready Edit
Medium (Copy) A medium is a material that light or other form of energy travels in or through. 0 Draft Edit
Medium (Copy) A medium is a material that light or other form of energy travels in or through. 0 Draft Edit
Mirror A mirror is an object that reflects light according to the law of reflection, or specular reflection. 0 Ready Edit
Mirror (Copy) A mirror is an object that reflects light according to the law of reflection, or specular reflection. 0 Draft Edit
MirrorCenterOfCurvatureRay For a spherical mirror, the center of curvature ray originates at the object, either passes through or is directed toward the center of curvature, and reflects straight back. 0 Ready Edit
MirrorCenterOfCurvatureRay (Copy) For a spherical mirror, the center of curvature ray originates at the object, either passes through or is directed toward the center of curvature, and reflects straight back. 0 Draft Edit
MirrorCenterOfCurvatureRay (Copy) (Copy) For a spherical mirror, the center of curvature ray originates at the object, either passes through or is directed toward the center of curvature, and reflects straight back. 0 Draft Edit
MirrorCenterOfCurvatureRay (Copy) (Copy) For a spherical mirror, the center of curvature ray originates at the object, either passes through or is directed toward the center of curvature, and reflects straight back. 0 Draft Edit
MirrorCentralRay For a mirror, the central ray originates at the object, travels to the center of the mirror and reflects. 0 Ready Edit
MirrorCentralRay (Copy) For a mirror, the central ray originates at the object, travels to the center of the mirror and reflects. 0 Draft Edit
MirrorLensApproximations for later: thin lens, spherical v parabolic surface, paraxial rays... 0 Draft Edit
MirrorLensApproximations (Copy) for later: thin lens, spherical v parabolic surface, paraxial rays... 0 Draft Edit
MirrorLensApproximations (Copy) (Copy) for later: thin lens, spherical v parabolic surface, paraxial rays... 0 Draft Edit
MirrorReflection Reflection from mirrors is specular reflection. 0 Ready Edit
MirrorReflection (Copy) Reflection from mirrors is specular reflection. 0 Draft Edit
MirrorReflection (Copy) (Copy) Reflection from mirrors is specular reflection. 0 Draft Edit
MirrorReflection (Copy) (Copy) Reflection from mirrors is specular reflection. 0 Draft Edit
MirrorThinLensEquation For mirrors and thin lenses, the relationship of the focal length $f$, object distance $d_\text{o}$, and image distance $d_\text{i}$ is $\frac{1}{d_\text{o}} + \frac{1}{d_\text{i}} = \frac{1}{f}$. 8 Ready Edit
MirrorThinLensEquation (Copy) For mirrors and thin lenses, the relationship of the focal length $f$, object distance $d_\text{o}$, and image distance $d_\text{i}$ is $\frac{1}{d_\text{o}} + \frac{1}{d_\text{i}} = \frac{1}{f}$. 0 Draft Edit
MirrorThinLensEquation (Copy) For mirrors and thin lenses, the relationship of the focal length $f$, object distance $d_\text{o}$, and image distance $d_\text{i}$ is $\frac{1}{d_\text{o}} + \frac{1}{d_\text{i}} = \frac{1}{f}$. 0 Draft Edit
MirrorThinLensEquation (Copy) (Copy) For mirrors and thin lenses, the relationship of the focal length $f$, object distance $d_\text{o}$, and image distance $d_\text{i}$ is $\frac{1}{d_\text{o}} + \frac{1}{d_\text{i}} = \frac{1}{f}$. 0 Draft Edit
MoonMass The Moon's mass is $7.34 \times 10^{22}$ kg. 0 Ready Edit
MoonMass (Copy) The Moon's mass is $7.34 \times 10^{22}$ kg. 0 Draft Edit
Motion An object's motion is its position at a series of times (clock readings). 0 Ready Edit
Motion (Copy) An object's motion is its position at a series of times (clock readings). 0 Draft Edit
Motion (Copy) (Copy) An object's motion is its position at a series of times (clock readings). 0 Draft Edit
Motion (Copy) (Copy) (Copy) An object's motion is its position at a series of times (clock readings). 0 Draft Edit
Motion (Copy) (Copy) (Copy) (Copy) An object's motion is its position at a series of times (clock readings). 0 Draft Edit
Motion (Copy) (Copy) (Copy) (Copy) (Copy) An object's motion is its position at a series of times (clock readings). 0 Draft Edit
Motion (Copy) (Copy) (Copy) (Copy) (Copy) An object's motion is its position at a series of times (clock readings). 0 Draft Edit
Motion (Copy) (Copy) (Copy) (Copy) (Copy) (Copy) An object's motion is its position at a series of times (clock readings). 0 Draft Edit
N2CompEquation The component of an object's acceleration in a particular direction is equal to the component of the net force in that direction, divided by the object's mass; $a_\text{x}= \frac{F_{\text{net,x}}}{m}$. 0 Ready Edit
N2CompEquation (Copy) The component of an object's acceleration in a particular direction is equal to the component of the net force in that direction, divided by the object's mass; $a_\text{x}= \frac{F_{\text{net,x}}}{m}$. 0 Draft Edit
NegAccelDecreasingVel An object having a negative component of acceleration in a particular direction during a time interval will have a lesser component of velocity in that direction at the end of the interval than at the beginning of the interval. 0 Ready Edit
NegAccelDecreasingVel (Copy) An object having a negative component of acceleration in a particular direction during a time interval will have a lesser component of velocity in that direction at the end of the interval than at the beginning of the interval. 0 Draft Edit
NegVelDecreasingPos The value of the position, on a particular axis, of an object having a negative velocity along that axis during a time interval will be less at the end of the interval than at the beginning. 0 Ready Edit
NegVelDecreasingPos (Copy) The value of the position, on a particular axis, of an object having a negative velocity along that axis during a time interval will be less at the end of the interval than at the beginning. 0 Draft Edit
NegVelDecreasingPos (Copy) (Copy) The value of the position, on a particular axis, of an object having a negative velocity along that axis during a time interval will be less at the end of the interval than at the beginning. 0 Draft Edit
NetForce The net force on an object is the sum of the individual forces acting on the object. 0 Ready Edit
NetForce (Copy) The net force on an object is the sum of the individual forces acting on the object. 0 Draft Edit
NetForce2Collinear Given two forces acting on an object along the same line, the net force on the object is (1) if the forces' directions are the same, a single force with magnitude equal to the sum of the forces' magnitudes and in the same direction (2) if the forces' directions are different and their magnitudes are different, a single force with magnitude equal to the difference of the two forces' magnitudes and in the direction of the stronger force (3) if the forces' directions are different and their magnitudes are the same, zero. 0 Ready Edit
NetForce2Collinear (Copy) Given two forces acting on an object along the same line, the net force on the object is (1) if the forces' directions are the same, a single force with magnitude equal to the sum of the forces' magnitudes and in the same direction (2) if the forces' directions are different and their magnitudes are different, a single force with magnitude equal to the difference of the two forces' magnitudes and in the direction of the stronger force (3) if the forces' directions are different and their magnitudes are the same, zero. 0 Draft Edit
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