Wize University Physics Textbook (Master) > Motion in Two Dimensions

The Position, Velocity, and Acceleration Vectors

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Position Vector (r) = fixed vector that locates a point in space relative to another point. Some call it the "distance" vector, as its magnitude is the distance between the endpoints.

  • can be used to form a unit vector
  • can be used to determine the length or distance between 2 points

IF USE THE ORIGIN AS THE STARTING POINT:

ex: so two points are O (0,0,0) and A (Ax, Ay, Az)


Image illustrating Position Vector


IF the ORIGIN is NOT the STARTING POINT:

ex: so two points are A (Ax, Ay, Az) and B (Bx, By, Bz), then rAB can be written as:


Image illustrating Position Vector


Image illustrating Position Vector



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Two- and Three-Dimensional Kinematics: Part 1


  • In general, the position of a particle is represented by a 3D vector that is changing with time. The components of this 3D vector are a function of time too.
r(t)⟶=x(t)ı^+y(t)ȷ^+z(t)k^\boxed{\stackrel{\longrightarrow}{r(t)}=x(t)\hat{\imath}+y(t)\hat{\jmath}+z(t)\hat k}




Image illustrating Two- and Three-Dimensional Kinematics : Part 1





  • Displacement is a vector that shows the change in position of the particle. The unit of displacement is m.


Δr⟶=rf→−rı^→=Δxı^+Δyȷ^+Δzk^\stackrel{\longrightarrow}{\Delta r}=\stackrel{\rightarrow}{r_f}-\stackrel{\rightarrow}{r_{\hat{\imath}}}=\Delta x\hat{\imath}+\Delta y\hat{\jmath}+\Delta z\hat k



  • Distance is the length of the path travelled by the particle




  • Average velocity is defined as


vave⟶=Δr⟶Δt\boxed{\stackrel{\longrightarrow}{v_{ave}}=\frac{\stackrel{\longrightarrow}{\Delta r}}{{\Delta t}}}







  • Instantaneous velocity is the velocity of an object in a specific time or position which in general might be different from the average velocity
v(t)⟶=vxı^+vyȷ^+vzk^=lim⁡Δt→0Δr⟶Δt=dr(t)⟶dt\stackrel{\longrightarrow}{v(t)}=v_x\hat{\imath}+v_y\hat{\jmath}+v_z\hat k=\lim_{\Delta t\to0}\frac{\stackrel{\longrightarrow}{\Delta r}}{{\Delta t}}=\frac{\stackrel{\longrightarrow}{dr(t)}}{{dt}}
dr(t)⟶dt=dx(t)dtı^+dy(t)dtȷ^+dz(t)dtk^\frac{\stackrel{\longrightarrow}{dr(t)}}{{dt}}=\frac{dx(t)}{dt}\hat{\imath}+\frac{dy(t)}{dt}\hat{\jmath}+\frac{dz(t)}{dt}\hat k
  • So, basically, the instantaneous velocity is obtained by taking the derivative of position with respect to time.




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Example: Position and Velocity

Given that the velocity of a body, starting from the origin, and moving along the x-axis, is v(t)=9.8t−5\displaystyle v(t)=9.8t-5, find the position of the moving body at t=3t=3.


Since the velocity is the derivative of position, position will be the integral of the velocity:


v(t)=dsdt=9.8t−5\displaystyle v\left(t\right)=\frac{ds}{dt}=9.8t-5


Integrate to find position:


s(t)=∫(9.8t−5) dt\displaystyle s(t)=\int{(9.8t-5)}\ dt


=9.82 t2−5t+C\displaystyle =\dfrac{9.8}{2}\ t^2-5t+C


Find the constant using the fact that the object starts at the origin, that is, position is zero when time is zero: s(0)=0s(0)=0. Put this in the equation to get:


0=9.82 (0)2−(0)t+C\displaystyle 0=\dfrac{9.8}{2} \ (0)^2-(0)t+C


⇒C=0\Rightarrow C=0


Therefore the position function is:


s(t)=9.82 t2−5t\displaystyle s(t)=\dfrac{9.8}{2}\ t^2-5t


At t=3t=3 the position is:


s(3)=(9.8)(9)2−5(3)s(3)=\dfrac{(9.8)(9)}{2}-5(3)


=29.1=\boxed{29.1}


Practice: Position Vectors

Given the points 𝑃(1,2), 𝑄(0,1),𝑃(1,2),\space 𝑄(0,1), and 𝑅(1,−1),𝑅(1,−1), find 𝑃𝑄→+𝑅𝑄→. \overrightarrow{𝑃𝑄}+ \overrightarrow{𝑅𝑄} .


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Example: Velocity and Acceleration in 3D


The position of a particle in 3D is given by

r⃗(t)=(10t+t2+7)i^+2j^+4tk^  m\vec{r}(t)=(10t+t^2+7)\hat{i}+2\hat{j}+4t\hat{k} \ \ m

a) Calculate instantaneous velocity at t =5 sec

b) Calculate the average velocity for an interval (3-5 sec).

c) Calculate the instantaneous acceleration at t =1 sec.


Solution:


Part a)


We know that Instantaneous velocity is

v⃗=dr⃗dt\vec{v} = \dfrac{d\vec{r}}{dt}


dr⃗dt=(10+2t)i^+0j^+4k^\frac{d\vec{r}}{dt}=(10+2t)\hat{i}+0\hat{j}+4\hat{k}


v⃗(t=5)=(10+2(5))i^+4k^=20i^+4k^ m/s\vec{v}(t=5)= (10 + 2 (5))\hat{i}+4\hat{k} = 20\hat{i}+4\hat{k} \ m/s


Part b)


Average velocity:


v⃗average=Δr⃗Δt=r⃗(5)−r⃗(3)5−3\vec{v}_{average}=\dfrac{\Delta\vec{r}}{\Delta t}=\dfrac{\vec{r}(5)-\vec{r}(3)}{5-3}


v⃗average=[82i^+2j^+20k^]−[46i^+2j^+12k^]2=36i^+8k^2=18i^+4k^ m/s\vec{v}_{average} = \dfrac{[82\hat{i}+2\hat{j}+20\hat{k}]-[46\hat{i}+2\hat{j}+12\hat{k}]}{2}=\dfrac{36\hat{i}+8\hat{k}}{2}= 18\hat{i}+4\hat{k}\ m/s


Part c)


Instantaneous acceleration:

a⃗instant=d2r⃗dt2=2i^ ms2\vec{a}_{instan t}=\dfrac{d^2\vec{r}}{dt^2}=2\hat{i} \ \dfrac{m}{s^2}





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Q:\textbf{Q:} A particle moves back and forth along a line such that it has a position function s=f(t)=t3−9t2+24ts=f(t)=t^3-9t^2+24t, where tt is measured in seconds and ss in meters. Find the velocity, speed and acceleration at t=5t=5.



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