EasyManua.ls Logo

HP 48GII - Angular Mechanics (4, 2); Centripetal Force (4, 3); Hookes Law (4, 4)

HP 48GII
653 pages
Print Icon
To Next Page IconTo Next Page
To Next Page IconTo Next Page
To Previous Page IconTo Previous Page
To Previous Page IconTo Previous Page
Loading...
Equation Reference 5-23
Angular Mechanics (4, 2)
Equations:
Example:
Given: I=1750_lb
∗
in^2,
Θ
=360_°, r=3.5_in, α=10.5_r/min^2,
ω
i=0_r / s.
Solution: r=1.1017E–3_ft_
∗
lbf, Ki=0_ft
∗
lbf, W=6.9221E–3_ft
∗
lbf, Kf=6.9221E–3_ft
∗
lbf,
at=8.5069E–4_ft/s^2, Ni=0_rpm,
ω
f=11.4868_r/min, t=1.0940_min, Nf=1.8282_rpm, Pavg=1.9174E–7_hp.
Centripetal Force (4, 3)
Equations:
Example:
Given: m=1_kg, r=5_cm, N=2000_Hz.
Solution:
ω
=12566.3706_r/s, ar=7895683.5209_m/s, F=7895683.5209_N, v=628.3185_m/s.
Hooke's Law (4, 4)
The force is that exerted by the spring.
Equations:
Fk–x⋅=
W
1–
2
------
kx
2
⋅⋅=
Example:
Given: k=1725_lbf/in, x=125_in.
Solution: F=-2156.25_lbf, W=-112.3047_ft
∗
lbf.
τ
I
α ⋅
= K i
1
2
- - -
I
ω
i
2
⋅ ⋅
=
K
f
1
2
- - -
I
ω
f
2
⋅ ⋅
=
W K
f
K i
–
=
ω
f
ω
i
α
+ t
⋅
=
P
τ
ω
⋅
=
P a v g
W
t
-----
=
W
r
Θ⋅
=
a
t
α
r
⋅
=
ω
f
2
π
N
f
⋅ ⋅
=
ω
2
π
N
⋅ ⋅
=
ω
i 2
π
N
i
⋅
⋅
=
F m
ω
2
r
⋅ ⋅
=
ω
2
π
N
⋅ ⋅
=
ω
v
r
- - -
=
a r
v
2
r
-----
=

Table of Contents