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2nd lecture notes Applied natural sciences (3NBB0) University Physics with Modern Physics, Global Edition, ISBN: 9781292314730 $3.21   Add to cart

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2nd lecture notes Applied natural sciences (3NBB0) University Physics with Modern Physics, Global Edition, ISBN: 9781292314730

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This document consists of the contents of the second lecture of applied natural sciences as it is taught in the mechanical engineering program.

Last document update: 3 year ago

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  • November 23, 2021
  • November 23, 2021
  • 2
  • 2021/2022
  • Class notes
  • Andre duif
  • College 2
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WAN HESS, ☒HNXIEEMYAATT 118$ HANK☒ DDYIINVAAMY118$
motion in two or three dimension
define coordinate system ( define origin & the ✗ -


, y -

,
and z-axis directions )
In 3D, determine position ( r ) at any moment in time

any position vector can be written as the sum of three vectors in the direction of each axis

trajectory : the path an object travels over time Fct) =
✗ (t ) it yet )j + 2 A) it
this requires you to find functions of change in position relative to each single axis over

time ( ✗ (t ) , y (t ) , 2- (t ) )
motion along a straight line can be used for each axis separately (axes are independant )

displacement and average velocity
displacement F' Ñ (ta) Flt ) : = -

.
= ri -
ri

using the definition of r→ in terms of the three axes :

(✗ a
-

✗ , )I + (ya -
) j + (Zz 2) ti
y , A ✗ i + ☐ yj - =
+ ☐z ti
Vaverage Crate of change position )
velocity
=
:




Vaverage = 2¥ it 1¥ É Varg I + Varg
j
+ =
-
✗ -

yj + Varg -
z
É
Vinstantaneous = ¥-70 %¥= 8¥ ¥ it dd¥J + ¥ É = =
✓✗ I + Vyjtvz E
this is the vector sum of instantaneous velocities in

the ✗
, y ,
and 2- directions

acceleration vector derivation similar to velocity :




instantaneous acceleration :
a→= ¥18 F¥=8¥ (time derivative of the velocity vector)

A.instantaneous :




= 8¥ : +8¥ ; +8¥ E
= a I + ayjtazk




vector sum of instantaneous accelerations in three directions

different way of looking at the acceleration vector

redefine velocity : ri ( magnitude ✗ direction)

✓ =
IF I =
vi. + Kit Vz
'




i = Tlv
a→=daY=a¥i +8¥
parallel acceleration : oi ,,
¥-0 =




normal to acceleration : at vd¥ =




applications :




projectiles (warfare and ball games)
circular motion (adventure parks)
projectile motion :




projectile objects :
that follow trajectory with given initial velocity determined by gravitation
(and air resistance)
'

a- (t) = 8¥ it -8¥ j -




projectile trajectory :




initial conditions E- 0 :




✗ =
0 , y = 0


Vox =
V0 COS do


Voy =
Vo sin do


y [✗ ) =
-

É9✗Y( V02 COST ao)) + tan (ao )

highest point ¥-0 Ymax Evo's in Tao )/g
=
:




distance of impact :
y =
0 ✗=0 or ✗ = R =
Voisin ( Zoro) 1g

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