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phy105 20221 midterm2 formula sheet

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PHY 105
FORMULA SHEET
Useful information:
Acceleration due to gravity:
𝑔 = 10 m/s2
Values of trigonometric functions for common angles:
sin30!
sin37!
sin45!
sin53!
sin60!
= 0.5, cos30!
= 0.6, cos37!
= 0.7, cos45!
= 0.8, cos53!
= 0.9, cos60!
= 0.9
= 0.8
= 0.7
= 0.6
= 0.5
Formulas:
Kinematic quantities (one-dimensional):
Δπ‘₯ = π‘₯" − π‘₯#
𝑣$,&'( =
)$
π‘Ž$,&'( =
)'!
)*
, 𝑣&'( =
)*
, π‘Ž$ =
+
)*
, 𝑣$ =
+$
+*
+'!
+*
Kinematic equations for constant acceleration
(one-dimensional):
𝑣$" = 𝑣$# + π‘Ž$ 𝑑
,
π‘₯" = π‘₯# + -9𝑣$# + 𝑣$" :𝑑
,
π‘₯" = π‘₯# + 𝑣$# 𝑑 + -π‘Ž$ 𝑑 𝑣$"
= 𝑣$#
+ 2π‘Ž$ 9π‘₯" − π‘₯# :
Kinematic quantities (multi-dimensional):
Δ𝒓
=βƒ— = =𝒓⃗" − =𝒓⃗#
/βƒ—
)𝒓
=βƒ—&'( = )* , 𝒗
𝒗
=βƒ— =
=βƒ— &'( =
𝒂
/βƒ—
)𝒗
)*
,𝒂
=βƒ— =
=βƒ—" = 𝒗
𝒗
=βƒ—# + =𝒂⃗𝑑
/βƒ—
+𝒓
,
+*
=βƒ—" = =𝒓⃗# + =𝒗⃗# 𝑑 + -=𝒂⃗𝑑 𝒓
/βƒ—
+𝒗
+*
Centripetal (radial) and tangential acceleration:
π‘Ž3 = π‘Ž4 =
'"
4
Kinematic equations for constant acceleration
(multi-dimensional):
+'
, π‘Ž* = A +* A
Period and frequency:
𝑇=
-54
'
,𝑓=
,
6
Newton’s second law:
Forces:
D =𝑭⃗ = π‘šπ’‚
=βƒ—
𝐹( = π‘šπ‘” (force of gravity)
𝑓7 ≤ πœ‡7 𝑛, 𝑓8 = πœ‡8 𝑛 (force of friction)
𝐹7 = −π‘˜π‘₯ (spring force; Hooke’s law)
Work:
Translational kinetic energy:
π‘Š = =𝑭⃗ βˆ™ Δ𝒓
=βƒ— = 𝐹Δπ‘Ÿ cos πœƒ (constant force)
𝐾 = -π‘šπ‘£ -
$
π‘Š = ∫$ # 𝐹$ 𝑑π‘₯ (varying force, one-dimensional)
$
,
Potential energy:
Work-kinetic energy theorem:
π‘ˆ( = π‘šπ‘”π‘¦ (gravitational)
π‘Š9:* = βˆ†πΎ
π‘ˆ7 = %"π‘˜π‘₯ - (elastic)
π‘Š#9* = −βˆ†π‘ˆ
𝐹$ = −&'
(one-dimensional)
&!
Conservation of mechanical energy:
Internal energy:
βˆ†πΈ;:3< = βˆ†πΎ + βˆ†π‘ˆ = 0
βˆ†πΈ#9* = 𝑓8 𝑑
Conservation of energy:
Power:
βˆ†πΈ7=7*:; = βˆ†πΎ + βˆ†π‘ˆ + βˆ†πΈ#9* = D π‘Š:$*
𝑃&'( = βˆ†)
, 𝑃&'( = +
βˆ†*
βˆ†*
βˆ†πΎ + βˆ†π‘ˆ = −𝑓8 𝑑 + D π‘Š:$*
Linear momentum:
𝑃 = &)
, 𝑃 = &+
&*
&*
Impulse:
*#
=βƒ— = π‘šπ’—
𝒑
=βƒ—
𝑰⃗ = βˆ†π’‘
=βƒ— = [ D =𝑭⃗ 𝑑𝑑
+𝒑
/βƒ—
+*
D =𝑭⃗ =
*$
Conservation of linear momentum:
Center of mass:
βˆ†π’‘
=βƒ—*!* = 0
=βƒ—?@ = ,% ∑# π‘š# =𝒓⃗# (system of particles)
𝒓
=βƒ—?@ = ,% ∫ =𝒓⃗ π‘‘π‘š (extended object)
𝒓
Angular kinematic quantities:
Δπœƒ = πœƒ" − πœƒ#
πœ”&'( =
)A
,πœ”=
)*
+A
𝛼&'( =
)B
+B
)*
,𝛼=
+*
+*
Rotational kinematic equations for constant angular
acceleration:
πœ”" = πœ”# + 𝛼𝑑
,
πœƒ" = πœƒ# + -9πœ”# + πœ”" :𝑑
,
πœƒ" = πœƒ# + πœ”# 𝑑 + -𝛼𝑑 πœ”"- = πœ”#- + 2𝛼9πœƒ" − πœƒ# :
Relationship between translational and angular
quantities:
𝑠 = π‘Ÿπœƒ
Torque:
𝜏 = π‘ŸπΉ sin πœ™ = 𝐹𝑑
𝑣 = π‘Ÿπœ”
π‘Ž* = π‘Ÿπ›Ό
Moment of inertia:
Newton’s second law for rotation:
𝐼 = ∑# π‘š# π‘Ÿ#- (system of particles)
D 𝜏 = 𝐼𝛼
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