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Fittoniya [83]
1 year ago
6

The robot arm is elevating and extending simultaneously. At a given instant, θ = 30°, ˙ θ = 10 deg / s = constant θ˙=10 deg/s=co

nstant , l = 0.5 m, ˙ l = 0.2 m / s l˙=0.2 m/s , and ¨ l = − 0.3 m / s 2 l¨=−0.3 m/s2 . Compute the magnitudes of the velocity v and acceleration a of the gripped part P. In addition, express v and a in terms of the unit vectors i and j.
Physics
1 answer:
motikmotik1 year ago
5 0

Explanation:

The position vector r:

\overrightarrow{r(t)}=lcos\theta\hat{i}+lsin\theta\hat{j}

The velocity vector v:

\overrightarrow{v(t)}=\overrightarrow{\frac{dr}{dt}}=\dot{l}cos\theta-lsin\theta\dot{\theta}\hat{i}+\dot{l}sin\theta+lcos\theta\dot{\theta}\hat{j}

The acceleration vector a:

\overrightarrow{a(t)}}=cos\theta(\ddot{l}-l\dot{\theta}^2)-sin\theta(2\dot{l}\dot{\theta}+l\ddot{\theta})\hat{i}+cos\theta(2\dot{l}\dot{\theta}+l\ddot{\theta})+sin\theta(\ddot{l}-l\dot{\theta}^2)\hat{j}

\overrightarrow{v(t)}=0.13\hat{i}+0.18\hat{j}

\overrightarrow{a(t)}}=-0.3\hat{i}-0.1\hat{j}

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Your film idea is about drones that take over the world. In the script, two drones are flying horizontally at the same speed and
Stella [2.4K]

Answer:

vₓ = 20 m/s,    v_{y}  = -15 m / s

Explanation:

This is a conservation of moment problem, since it is a vector quantity we can work each axis independently

The system is formed by the two drones, so the forces during the crash are internal and the moment is conserved

X axis

Initial moment. Before the crash

         p₀ = m₁ v₀ₓ + m₂ v₀ₓ

Final moment. After the crash

       p_{fx} = (m₁ + m₂) vₓ

      p₀ₓ = p_{fx}

      m₁ v₀ₓ + m₂ v₀ₓ = (m₁ + m₂) vₓ

       vₓ = (m₁ + m₂) v₀ₓ / (m₁ + m₂)

       vₓ = v₀ₓ  = 20 m/s

Y Axis

Initial

         p_{oy} = m₁ v_{oy}

Final

         p_{fy} = (m₁ + m₂) v_{y}

         p_{oy} = p_{fy}

the drom rises and when it falls it has the same speed because there is no friction    v_{oy} = -60 m/s          

 

           m₁ v_{oy} = (m₁ + m₂) v_{y}

            v_{y} = m₁ / (m₁ + m₂) v_{oy}

            v_{y}  = 1/4    60

            v_{y}  = -15 m / s

Vertical speed is down

5 0
2 years ago
Suppose I have an infinite plane of charge surrounded by air. What is the maximum charge density that can be placed on the surfa
gregori [183]

Answer:

53.1\mu C/m^2

Explanation:

We are given that

Electric field,E=3\times 10^6V/m

We have to find the value of maximum charge density that can be placed on the surface of the plane before dielectric breakdown of the surrounding air occurs.

We know that

E=\frac{\sigma}{2\epsilon_0}

Where \epsilon_0=8.85\times 10^{-12}

Using the formula

3\times 10^6=\frac{\sigma}{2\times 8.85\times 10^{-12}}

\sigma=3\times 10^6\times 2\times 8.85\times 10^{-12}

\sigma=5.31\times 10^{-5}C/m^2

\sigma=53.1\times 10^{-6}C/m^2=53.1\mu C/m^2

1\mu C=10^{-6} C

3 0
2 years ago
A bullet starting from rest accelerates uniformly at a rate of 1,250 meters per square second. What is the bullet's speed after
Tatiana [17]

Answer:

125,000

Explanation:

8 0
2 years ago
A certain heat engine extracts 1.30 kJ of heat from a hot temperature reservoir and discharges 0.70 kJ of heat to a cold tempera
skelet666 [1.2K]

Answer:

46%  (0.46)

Explanation:

temperature of hot reservoir (Th) = 1.3 kJ

temperature of COLD reservoir (Tc) = 0.7 kJ

Efficiency = 1 - (Tc/Th)

Efficiency = 1 - (0.7/1.3) = 0.46 = 0.46 x 100 = 46 %

7 0
1 year ago
Read 2 more answers
What tangential speed, v, must the bob have so that it moves in a horizontal circle with the string always making an angle θ fro
Rainbow [258]

Answer:

v = √(Lsinθ tanθ)

Explanation:

From the diagram attached,

v = the tangential speed.

r = the radius of the horizontal circle.

T = tension in the string.

θ =  the angle that the string makes with the vertical

m =  Bob's mass  (mg = the weight)

F =  centripetal force

L = the length of the string

From geometry,

r = Lsin θ

Thus, the centripetal acceleration is given as;

a = v²/r = v²/Lsin θ

Force = mass x acceleration

Thus,

Centripetal force = mv²/Lsin θ

Let's balance the vertical forces to obtain,

T cosθ - mg = 0

Thus, T cosθ = mg - - - - (eq1)

Similarly, let's balance the horizontal forces to obtain;

T sinθ = F = mv²/Lsin θ

So, T sinθ = mv²/Lsin θ - - - - (eq2)

Let's divide eq 2 by eq 1 to get;

Tsinθ/Tcosθ = (mv²/Lsin θ)/mg

tanθ = gv²/Lsinθ

Thus, v² =  Lsinθ tanθ

v = √(Lsinθ tanθ)

4 0
1 year ago
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