Apply Second Newton's Law to mass m1 :
in the x direction
m 1 ⋅ a = T − f 1 = { f 1 = μ 1 ⋅ F n 1 } = T − μ 1 ⋅ F n 1 ( 1 ) m_1 \cdot a=T-f_1=\{ f_1=\mu _1 \cdot Fn_1 \}=T-\mu _1 \cdot Fn_1 \space (1) m 1 ⋅ a = T − f 1 = { f 1 = μ 1 ⋅ F n 1 } = T − μ 1 ⋅ F n 1 ( 1 ) in the y direction
0 = F n 1 − m 1 ⋅ g ( 2 ) 0=Fn_1 -m_1 \cdot g \space (2) 0 = F n 1 − m 1 ⋅ g ( 2 ) From (1) and (2):
T = m 1 ⋅ a + μ 1 ⋅ m 1 ⋅ g ( 3 ) T = m_1 \cdot a + \mu_1 \cdot m_1 \cdot g \space (3) T = m 1 ⋅ a + μ 1 ⋅ m 1 ⋅ g ( 3 ) Apply Second Newton's Law to mass m2 :
in the x direction
m 2 ⋅ a ⋅ c o s 3 0 ∘ = − T ⋅ c o s 3 0 ∘ − f 2 ⋅ c o s 3 0 ∘ + F n 2 ⋅ s i n 3 0 ∘ m_2 \cdot a \cdot cos30^ \circ=-T \cdot cos30^ \circ - f_2 \cdot cos30^ \circ + Fn_2 \cdot sin30^ \circ m 2 ⋅ a ⋅ cos 3 0 ∘ = − T ⋅ cos 3 0 ∘ − f 2 ⋅ cos 3 0 ∘ + F n 2 ⋅ s in 3 0 ∘ f 2 = μ 2 ⋅ F n 2 → m 2 ⋅ a = − T + F n 2 ⋅ ( 1 / 3 − μ 2 ) ( 4 ) f_2 = \mu_2 \cdot Fn_2 \space \rightarrow \space m_2 \cdot a =-T + Fn_2 \cdot (1/ \sqrt{3} - \mu_2) \space (4) f 2 = μ 2 ⋅ F n 2 → m 2 ⋅ a = − T + F n 2 ⋅ ( 1/ 3 − μ 2 ) ( 4 ) in the y direction
− m 2 ⋅ a ⋅ s i n 3 0 ∘ = T ⋅ s i n 3 0 ∘ + f 2 ⋅ s i n 3 0 ∘ + F n 2 ⋅ c o s 3 0 ∘ − m 2 ⋅ g -m_2 \cdot a \cdot sin30^ \circ=T \cdot sin30^ \circ + f_2 \cdot sin30^ \circ + Fn_2 \cdot cos30^ \circ - m_2 \cdot g − m 2 ⋅ a ⋅ s in 3 0 ∘ = T ⋅ s in 3 0 ∘ + f 2 ⋅ s in 3 0 ∘ + F n 2 ⋅ cos 3 0 ∘ − m 2 ⋅ g − m 2 ⋅ a = T + F n 2 ⋅ ( 3 + μ 2 ) − 2 ⋅ m 2 ⋅ g ( 5 ) -m_2 \cdot a =T + Fn_2 \cdot (\sqrt{3}+\mu_2) - 2 \cdot m_2 \cdot g \space (5) − m 2 ⋅ a = T + F n 2 ⋅ ( 3 + μ 2 ) − 2 ⋅ m 2 ⋅ g ( 5 ) From (4) and (5):
− m 2 ⋅ a = T + ( m 2 ⋅ a + T ) 3 + μ 2 1 / 3 − μ 2 − 2 ⋅ m 2 ⋅ g -m_2 \cdot a =T + (m_2 \cdot a +T) \frac {\sqrt{3}+\mu_2} {1/ \sqrt{3} - \mu_2} - 2 \cdot m_2 \cdot g − m 2 ⋅ a = T + ( m 2 ⋅ a + T ) 1/ 3 − μ 2 3 + μ 2 − 2 ⋅ m 2 ⋅ g a = g m 1 + m 2 ( m 2 2 ( 1 − 3 ⋅ μ 2 ) − μ 1 ⋅ m 1 ) a=\frac g {m_1+m_2} \Big( \frac {m_2} {2} (1-\sqrt{3} \cdot \mu_2)-\mu_1 \cdot m_1 \Big) a = m 1 + m 2 g ( 2 m 2 ( 1 − 3 ⋅ μ 2 ) − μ 1 ⋅ m 1 ) a = 9.81 m / s 2 3 k g + 4 k g ( 4 k g 2 ( 1 − 3 ⋅ 0.1 ) − 0.3 ⋅ 3 k g ) ≅ 1.06 m s 2 a=\frac {9.81 m/s^2} {3 kg+4 kg} \Big( \frac {4 kg} {2} (1-\sqrt{3} \cdot 0.1 ) - 0.3 \cdot 3kg \Big) \cong 1.06 \frac {m} {s^2} a = 3 k g + 4 k g 9.81 m / s 2 ( 2 4 k g ( 1 − 3 ⋅ 0.1 ) − 0.3 ⋅ 3 k g ) ≅ 1.06 s 2 m From (3):
T = m 1 ⋅ a + μ 1 ⋅ m 1 ⋅ g = 3 k g ⋅ 1.06 m / s 2 + 0.3 ⋅ 3 k g ⋅ 9.81 m / s 2 ≅ 11.997 N T = m_1 \cdot a + \mu_1 \cdot m_1 \cdot g = 3kg \cdot 1.06 m/s^2 + 0.3 \cdot 3kg \cdot 9.81 m/s^2 \cong 11.997 N T = m 1 ⋅ a + μ 1 ⋅ m 1 ⋅ g = 3 k g ⋅ 1.06 m / s 2 + 0.3 ⋅ 3 k g ⋅ 9.81 m / s 2 ≅ 11.997 N Answer:
T ≅ 12 N , a ≅ 1 m / s 2 T \cong 12 N ,\space \space a \cong 1m/s^2 T ≅ 12 N , a ≅ 1 m / s 2
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