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Olegator [25]
3 years ago
14

Balance the equationP + 02 → P205 ​

Physics
2 answers:
AlladinOne [14]3 years ago
6 0

Answer:

<u>4</u>P + <u>5</u>02 → <u>2</u>P205

Explanation:

Hence the above equation is balanced.

ivolga24 [154]3 years ago
3 0

Explanation:

\underline{ \underline{ \large{ \text{Given \: chemical \: equation}}}} :

  • \tt{P \:  + O _{2} \: \:  \:  \: ➞ \:  \:  P_{2} \: O_{5}}

Here , Multiply P2O5 by 2 and O2 by 5 to equalize oxygen :

\tt{P+ 5O_{2} \:  \:  ➞\:  \: 2P_{2} \:O_{5}}

Now , To equalize P atoms , Multiply P by 4

\boxed{  \large{\tt{ 4P + 5O _{2} \: ➞ \:   \:  \: \: 2P_{2} \: O_{5}}}}

Here , On the left side we have 4P and On the right side ,we have 4P. Again , On the left side , we have 10 O and On the right side , we have 10 O. And yippie , we got the balanced chemical equation !!!

Hope I helped ! ♡

Have a wonderful day / night ! ツ

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Calculate the magnitude of the acceleration of the box if you push on the box with a constant force 170.0 N that is parallel to
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The acceleration of the  box up the ramp is 9.65 m/s².

<h3>What is the magnitude of acceleration of the box?</h3>

The magnitude of the acceleration of the box is calculated by applying Newton's second law of motion as shown below;

F(net) = ma

where;

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  • a is the acceleration of the box

The net force on the box is calculated as follows;

F(net) = F - Ff

F(net) = F - μmgcosθ

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F(net) = 170 -  (0.3 x 15 x 9.8 x cos55)

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8 0
1 year ago
A uniform beam with mass M and length L is attached to the wall by a hinge, and supported by a cable. A mass of value 3M is susp
Jobisdone [24]

Answer:

The tension is  T= \frac{11}{2\sqrt{3} } Mg

The horizontal force provided by hinge   Fx= \frac{11}{4\sqrt{3} } Mg

Explanation:

   From the question we are told that

          The mass of the beam  is   m_b =M

          The length of the beam is  l = L

           The hanging mass is  m_h = 3M

            The length of the hannging mass is l_h = \frac{3}{4} l

            The angle the cable makes with the wall is \theta = 60^o

The free body diagram of this setup is shown on the first uploaded image

The force F_x \ \ and \ \ F_y are the forces experienced by the beam due to the hinges

      Looking at the diagram we ca see that the moment of the force about the fixed end of the beam along both the x-axis and the y- axis is zero

     So

           \sum F =0

Now about the x-axis the moment is

              F_x -T cos \theta  = 0

     =>     F_x = Tcos \theta

Substituting values

            F_x =T cos (60)

                 F_x= \frac{T}{2} ---(1)

Now about the y-axis the moment is  

           F_y  + Tsin \theta  = M *g + 3M *g ----(2)

Now the torque on the system is zero because their is no rotation  

   So  the torque above point 0 is

          M* g * \frac{L}{2}  + 3M * g \frac{3L}{2} - T sin(60) * L = 0

            \frac{Mg}{2} + \frac{9 Mg}{4} -  T * \frac{\sqrt{3} }{2}    = 0

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               T = \frac{11Mg}{4} * \frac{2}{\sqrt{3} }

                   T= \frac{11}{2\sqrt{3} } Mg

The horizontal force provided by the hinge is

             F_x= \frac{T}{2} ---(1)

Now substituting for T

              F_{x} = \frac{11}{2\sqrt{3} } * \frac{1}{2}

                  Fx= \frac{11}{4\sqrt{3} } Mg

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