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Gnesinka [82]
3 years ago
12

At t = 0, a wheel rotating about a fixed axis at a constant angular acceleration of -0. 40 rad/s2 has an angular velocity of 1.

5 rad/s and an angular position of 2. 3 rad. What is the angular position of the wheel at t = 2. 0 s?.
Physics
1 answer:
Novay_Z [31]3 years ago
8 0

The angular position of the wheel at t = 2. 0 s is 4.5 rad.

Angular Position:

When an object is undergoing a rotational motion, then the orientation of the object with respect to a specific reference position is known as angular position.

Given data:

The angular acceleration of the object at initial is, α = - 0.40 rad/s².

The angular velocity of the object is, ω = 1.5 rad/s.

The angular position of the object at initial is, \theta = 2.3 \;\rm rad.

The time interval is, t = 2.0 s.

The expression for the angular position of the wheel at t = 2.0 s is,

\theta' = \theta+ \omega t + \dfrac{1}{2} \alpha t^{2}

Solving as,

\theta' = 2.3+ (1.5 \times 2) + \dfrac{1}{2} \times (-0.40) \times 2^{2}\\\\
\theta' = 4.5 \;\rm rad

Thus, we can conclude that the angular position of the wheel at t = 2. 0 s is 4.5 rad.

Learn more about the angular position here:

brainly.com/question/6226195

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An electric field of 100 V/m is directed outward from the plane of a circular area with radius 4.0 cm. If the electric field inc
Flura [38]

Answer:

The magnitude of the magnetic field is 8.9\times10^{-19}\ T

Explanation:

Given that,

Electric field = 100 V/m

Radius = 4.0 cm

Electric field increase at a rate = 10 V/ms

Radial distance = 10.0 cm

We need to calculate the magnetic field

Using Gauss's law

\oint{\vec{E}\cdot\vec{dA}}=\phi_{E}

\dfrac{dE}{dt}A=\dfrac{d\phi_{E}}{dt}

\dfrac{dE}{dt}(\pi r^2)=\dfrac{d\phi_{E}}{dt}

We need to calculate the \dfrac{d\phi}{dt}

\dfrac{d\phi}{dt}=10\times\pi\times(4.0\times10^{-2})^2

\dfrac{d\phi}{dt}=0.0503\ Nm^2/C.s

According to Ampere Maxwell law

\oint{\vec{B}\cdot \vec{ds}}=\mu_{0}(I+\epsilon_{0}\dfrac{d\phi_{E}}{dt})

\oint{\vec{B}\cdot\vec{ds}}=\mu_{0}I+\mu_{0}\epsilon_{0}\dfrac{d\phi_{E}}{dt})

Electric field is zero inside the circle.

\oint{\vec{B}\cdot \vec{ds}}=\mu_{0}\epsilon_{0}\dfrac{d\phi_{E}}{dt})

B(2\pi\times10.0\times10^{-2})=4\pi\times10^{-7}\times8.85\times10^{-12}\times0.0503

B=\dfrac{4\pi\times10^{-7}\times8.85\times10^{-12}\times0.0503}{2\pi\times10.0\times10^{-2}}

B=8.9\times10^{-19}\ T

Hence, The magnitude of the magnetic field is 8.9\times10^{-19}\ T

6 0
3 years ago
If the baseball and the plastic ball were moving at the same speed which ball would hit a bat harder
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A baseball would hit the bat harder. This is because the baseball is a lot heavier and more dense than the plastic ball. The keyword that you're looking for is density. The baseball is dense.
7 0
4 years ago
A 2.3 m long wire weighing 0.075 N/m is suspended directly above an infinitely straight wire. The top wire carries a current of
ZanzabumX [31]

Answer:

Explanation:

Magnetic field near current carrying wire

= \frac{\mu_0}{4\pi} \frac{2i}{r}

i is current , r is distance from wire

B =  10⁻⁷ x \frac{2\times49}{r}

force on second wire per unit length

B I L , I is current in second wire , L is length of wire

=  10⁻⁷ x \frac{2\times49}{r} x 33 x 1

= 3234 x \frac{10^{-7}}{r}

This should balance weight of second wire per unit length

3234 x \frac{10^{-7}}{r} = .075

r = \frac{3234}{.075} x 10⁻⁷

= .0043 m

= .43 cm .

5 0
4 years ago
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3 years ago
Using the force table, components of a vector can be found experimentally by suspending masses from 2 orthogonal strings which o
SCORPION-xisa [38]
Answer: 134.23g at 0° (horizontal) and 77.5g at 90° (vertical).

Explanation:

1) Since the mass of <span>155 g is suspended at 210 degrees, you need to find the components of its weight on the orthogonal coordinate system (0° and 90°).
</span>

<span>2) You do that using the trignometric ratios sine and cosine.
</span>

<span>Weight is mass × g.
</span>
<span>Weight of the object = 155g × g
</span>
<span>Angle, α = 210°
</span>

<span>Horizontal component (0°)
</span>
<span>cosα = horizontal / hypotenuse ⇒ horizontal = hypotenuse × cosα
</span>
⇒ horizontal = 155g × g × cos(210°) = - 134.23g  × g

Vertical component
sinα = vertical / hypotenuse ⇒ vertical = hypotenuse × sinα
⇒ vertical = 155g × g × sin(210°) = -77.5g × g

3) Conclusion:

Therefore, the masses that must be suspended to balance the forces of the 155g mass are 134.23g at 0° (horizontal) and 77.5g at 90° (vertical).




8 0
3 years ago
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