HK. Newton I
V = S / t -> a = 0
a = F / m
m > -> F >
dalam HK. Newton II
V tdk = V0 -> a tdk = 0
GLB : momentum linier
P = m . V
= m . delta S / delta t
P = momentum
F = m . a -> m = F / a
P = (F / a) . (delta S / delta t)
= (F / delta V / delta t) . (delta S / delta t)
= ( F / delta V) . delta S
= (F / delta S / delta t) . delta S
P = F . delta t
Gaya gesek pada bidang horizontal
fs = Us . N ; fk = Uk . N ; N = W = m . g
benda diam F < fs
benda tetap akan bergerak
Macam-macam gaya (N / Newton)
V = S / t -> a = 0
a = F / m
m > -> F >
dalam HK. Newton II
V tdk = V0 -> a tdk = 0
- untuk merubah V, butuh a
- untuk menghasilkan a, butuh F sebanding m
GLB : momentum linier
P = m . V
= m . delta S / delta t
P = momentum
F = m . a -> m = F / a
P = (F / a) . (delta S / delta t)
= (F / delta V / delta t) . (delta S / delta t)
= ( F / delta V) . delta S
= (F / delta S / delta t) . delta S
P = F . delta t
Gaya gesek pada bidang horizontal
fs = Us . N ; fk = Uk . N ; N = W = m . g
benda diam F < fs
benda tetap akan bergerak
Macam-macam gaya (N / Newton)
- Gaya ( F ) -> Force
- Gaya berat (W) -> weight
- Gaya gesek ( f ) -> friction
- Tegang Tali (T) -> Tension
Sumbu x
Fx = fx - Nx
Sumbu y
Fy = Ny + fy - W
Hubungan gaya :
- F & m -> a
- F & t -> P
- F & S -> W (work / kerja)
Gaya Kerja pd benda
W = F . delta S
W = m . a . s => klo m a s harus work
Kerja perlu energi / tenaga : ada 2 energi
energi mekanik :energi gerak -> energi mekanik
- kecepatan -> E. Kinetik -> Ek = 1/2 m V^2
- Posisi -> E.Potensial -> Ep = m . g . h
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