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Displacement (geometry)

From Wikipedia, the free encyclopedia
(Redirected fromDisplacement (vector))
Vector relating the initial and the final positions of a moving point
For other uses, seeDisplacement (disambiguation).
Displacement
Displacement versus distance travelled along a path
Common symbols
d,s, ∆s , ∆x , ∆y, ∆z
SI unitmetre
InSI base unitsm
DimensionL
Part of a series on
Classical mechanics
F=dpdt{\displaystyle {\textbf {F}}={\frac {d\mathbf {p} }{dt}}}

Ingeometry andmechanics, adisplacement is avector whose length is the shortestdistance from the initial to the finalposition of a point P undergoingmotion.[1] It quantifies both the distance anddirection of the net or total motion along a straight line from the initial position to the final position of the pointtrajectory. A displacement may be identified with thetranslation that maps the initial position to the final position. Displacement is the shift in location when an object in motion changes from one position to another.[2]For motion over a given interval of time, the displacement divided by the length of the time interval defines theaverage velocity (a vector), whose magnitude is theaverage speed (a scalar quantity).

Formulation

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A displacement may be formulated as arelative position (resulting from the motion), that is, as the final positionxf of a point relative to its initial positionxi. The corresponding displacement vector can be defined as thedifference between the final and initial positions:s=xfxi=Δx{\displaystyle s=x_{\textrm {f}}-x_{\textrm {i}}=\Delta {x}}

Rigid body

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In dealing with the motion of arigid body, the termdisplacement may also include therotations of the body. In this case, the displacement of a particle of the body is calledlinear displacement (displacement along a line), while the rotation of the body is calledangular displacement.[3]

Derivatives

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See also:Position (geometry) § Derivatives

For a position vectors{\displaystyle \mathbf {s} } that is a function of timet{\displaystyle t}, the derivatives can be computed with respect tot{\displaystyle t}. The first two derivatives are frequently encountered in physics.

Velocity
v=dsdt{\displaystyle \mathbf {v} ={\frac {d\mathbf {s} }{dt}}}
Acceleration
a=dvdt=d2sdt2{\displaystyle \mathbf {a} ={\frac {d\mathbf {v} }{dt}}={\frac {d^{2}\mathbf {s} }{dt^{2}}}}
Jerk
j=dadt=d2vdt2=d3sdt3{\displaystyle \mathbf {j} ={\frac {d\mathbf {a} }{dt}}={\frac {d^{2}\mathbf {v} }{dt^{2}}}={\frac {d^{3}\mathbf {s} }{dt^{3}}}}

These common names correspond to terminology used in basic kinematics.[4] By extension, the higher order derivatives can be computed in a similar fashion. Study of these higher order derivatives can improve approximations of the original displacement function. Such higher-order terms are required in order to accurately represent the displacement function asa sum of an infinite series, enabling several analytical techniques in engineering and physics. The fourth order derivative is calledjounce.

Discussion

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In considering motions of objects over time, the instantaneousvelocity of the object is the rate of change of the displacement as a function of time. The instantaneousspeed, then, is distinct from velocity, or thetime rate of change of the distance travelled along a specific path. The velocity may be equivalently defined as the time rate of change of the position vector. If one considers a moving initial position, or equivalently a moving origin (e.g. an initial position or origin which is fixed to a train wagon, which in turn moves on its rail track), the velocity of P (e.g. a point representing the position of a passenger walking on the train) may be referred to as arelative velocity; this is opposed to anabsolute velocity, which is computed with respect to a point and coordinate axes which are considered to be at rest (ainertial frame of reference such as, for instance, a point fixed on the floor of the train station and the usual vertical and horizontal directions).

See also

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References

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  1. ^Tom Henderson."Describing Motion with Words".The Physics Classroom. Retrieved2 January 2012.
  2. ^Moebs, William; Ling, Samuel J.; Sanny, Jeff (2016-09-19)."3.1 Position, Displacement, and Average Velocity - University Physics Volume 1 | OpenStax".openstax.org. Retrieved2024-03-11.
  3. ^"Angular Displacement, Velocity, Acceleration".NASA Glenn Research Center. National Aeronautics and Space Administration. 13 May 2021. Retrieved9 November 2023.
  4. ^Stewart, James (2001). "§2.8 - The Derivative As A Function".Calculus (2nd ed.). Brooks/Cole.ISBN 0-534-37718-1.

External links

[edit]
Linear/translational quantitiesAngular/rotational quantities
Dimensions1LL2Dimensions1θθ2
Ttime:t
s
absement:A
m s
Ttime:t
s
1distance:d,position:r,s,x,displacement
m
area:A
m2
1angle:θ,angular displacement:θ
rad
solid angle:Ω
rad2, sr
T−1frequency:f
s−1,Hz
speed:v,velocity:v
m s−1
kinematic viscosity:ν,
specific angular momentumh
m2 s−1
T−1frequency:f,rotational speed:n,rotational velocity:n
s−1,Hz
angular speed:ω,angular velocity:ω
rad s−1
T−2acceleration:a
m s−2
T−2rotational acceleration
s−2
angular acceleration:α
rad s−2
T−3jerk:j
m s−3
T−3angular jerk:ζ
rad s−3
Mmass:m
kg
weighted position:Mx⟩ = ∑mxmoment of inertiaI
kg m2
ML
MT−1Mass flow rate:m˙{\displaystyle {\dot {m}}}
kg s−1
momentum:p,impulse:J
kg m s−1,N s
action:𝒮,actergy:
kg m2 s−1,J s
MLT−1angular momentum:L,angular impulse:ΔL
kg m rad s−1
MT−2force:F,weight:Fg
kg m s−2,N
energy:E,work:W,Lagrangian:L
kg m2 s−2,J
MLT−2torque:τ,moment:M
kg m rad s−2,N m
MT−3yank:Y
kg m s−3, N s−1
power:P
kg m2 s−3W
MLT−3rotatum:P
kg m rad s−3, N m s−1
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