t = 0.527 s
<u>It accelerates for 0.527 s.</u>
<u>Explanation:</u>
We use the formula:
v = u+at
Given:
v = 106 m/s
u = 0 (since no gravity)
![a=201 \mathrm{m} / \mathrm{s}^{2}](https://tex.z-dn.net/?f=a%3D201%20%5Cmathrm%7Bm%7D%20%2F%20%5Cmathrm%7Bs%7D%5E%7B2%7D)
So applying the formula,
v = u+at
106 = 0 + 201t
t = 106/201
t = 0.527 s
Answer:
h' = 55.3 m
Explanation:
First, we analyze the horizontal motion of the projectile, to find the time taken by the arrow to reach the orange. Since, air friction is negligible, therefore, the motion shall be uniform:
s = vt
where,
s = horizontal distance between arrow and orange = 60 m
v = initial horizontal speed of the arrow = v₀ Cos θ
θ = launch angle = 30°
v₀ = launch speed = 35 m/s
Therefore,
60 m = (35 m/s)Cos 30° t
t = 60 m/30.31 m/s
t = 1.98 s
Now, we analyze the vertical motion to find the height if arrow at this time. Using second equation of motion:
h = Vi t + (1/2)gt²
where,
Vi = Vertical Component of initial Velocity = v₀ Sin θ = (35 m/s)Sin 30°
Vi = 17.5 m/s
Therefore,
h = (17.5 m/s)(1.98 s) + (1/2)(9.81 m/s²)(1.98 s)²
h = 34.6 m + 19.2 m
h = 53.8 m
since, the arrow initially had a height of y = 1.5 m. Therefore, its final height will be:
h' = h + y
h' = 53.8 m + 1.5 m
<u>h' = 55.3 m</u>
Answer:
W = 30 N
Explanation:
Applying the summation of torques about the wedge for equilibrium, taking the clockwise direction as negative. Since the ruler is balanced horizontally about the wedge. Therefore, the summation of all torques acting about the wedge must be equal to zero.
![(70\ N)(40\ cm - 10\ cm)-(30\ N)(50\ cm-40\ cm)-(W)(100\ cm - 40\ cm) = 0\\W(60\ cm) = (70\ N)(30\ cm)-(30\ N)(10\ cm)\\\\W = \frac{1800\ N.cm}{60\ cm}](https://tex.z-dn.net/?f=%2870%5C%20N%29%2840%5C%20cm%20-%2010%5C%20cm%29-%2830%5C%20N%29%2850%5C%20cm-40%5C%20cm%29-%28W%29%28100%5C%20cm%20-%2040%5C%20cm%29%20%3D%200%5C%5CW%2860%5C%20cm%29%20%3D%20%2870%5C%20N%29%2830%5C%20cm%29-%2830%5C%20N%29%2810%5C%20cm%29%5C%5C%5C%5CW%20%3D%20%5Cfrac%7B1800%5C%20N.cm%7D%7B60%5C%20cm%7D)
<u>W = 30 N</u>
Answer:
(D) F/2
Explanation:
Since the circular section is unbanked, the centripedal acceleration acting on each of the cars is
![a_s = \frac{v_s^2}{r} = \frac{(2v)^2}{r} = \frac{4v^2}{r}](https://tex.z-dn.net/?f=a_s%20%3D%20%5Cfrac%7Bv_s%5E2%7D%7Br%7D%20%3D%20%5Cfrac%7B%282v%29%5E2%7D%7Br%7D%20%3D%20%5Cfrac%7B4v%5E2%7D%7Br%7D)
![a_l = \frac{v_l^2}{r} = \frac{v^2}{r}](https://tex.z-dn.net/?f=a_l%20%3D%20%5Cfrac%7Bv_l%5E2%7D%7Br%7D%20%3D%20%5Cfrac%7Bv%5E2%7D%7Br%7D)
Therefore the centripetal force on each car
![F_s = m_sa_s = \frac{4mv^2}{r}](https://tex.z-dn.net/?f=F_s%20%3D%20m_sa_s%20%3D%20%5Cfrac%7B4mv%5E2%7D%7Br%7D)
![F_l = m_la_l = \frac{2mv^2}{r}](https://tex.z-dn.net/?f=F_l%20%3D%20m_la_l%20%3D%20%5Cfrac%7B2mv%5E2%7D%7Br%7D)
Since
this means the friction force required to keep the large car on the road is only half of the friction force required to keep the small car on road
So (D) F/2 is the correct answer