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Helen [10]
3 years ago
15

A charge 3q is at the origin, and a charge −2q is on the positive x axis at x=a. part a where on the x-axis would you place a th

ird charge so it would experience no net electric force? enter an expression for the exact answer, which will involve a square-root sign. (do not enter an approximate decimal answer.)
Physics
1 answer:
Mila [183]3 years ago
6 0

Answer:

x = a + \frac{a\sqrt2}{\sqrt3 - \sqrt2}

Explanation:

Position of charge 3q is x = 0

position of charge -2q is x = a

so here we know that

when two charges are of opposite nature then the electric field will be zero on the line joining the two charges at the position near to smaller magnitude charge

So here the electric field will be zero if the field due to 3q is counterbalanced by field due to -2q

so here we can say

\frac{k(3q)}{(r+a)^2} + \frac{k(-2q)}{r^2} = 0

\frac{3}{(r + a)^2} = \frac{2}{r^2}

\frac{r+a}{r} = \sqrt{\frac{3}{2}}

1 + \frac{a}{r} =\sqrt{\frac{3}{2}}

\frac{a}{r} = \frac{\sqrt3 - \sqrt2}{\sqrt2}

so we will have

r = \frac{a\sqrt2}{\sqrt3 - \sqrt2}

so the x coordinate of this position is given as

x = a + \frac{a\sqrt2}{\sqrt3 - \sqrt2}

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Explain the difference between voluntary and involuntary muscles.
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How do electromagnetic waves differ from mechanical waves?
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An electric ceiling fan is rotating about a fixed axis with an initial angular velocity magnitude of 0.250rev/s . The magnitude
solmaris [256]

Answer:

1

The fan's angular velocity w_f =0.43\ rev /s

2

The number of turns is \theta = 0.0652\ rev

3

  The tangential speed v_t = 1.06 m/s

4

The  magnitude a of the resultant acceleration a_r = 3.6 m/s^2

Explanation:

From the question we are given that

         The initial angular velocity is w_{in} = 0.250 \ rev/s

          The angular acceleration is \alpha  = 0.891 \ rev/s^2

          The diameter of the ceiling fan blades d=0.800\ m

The diagram for this motion is shown on the first uploaded image

The motion involved in this problem statement is rotational motion and this motion can be defined in terms of angular velocity , angular displacement and angular acceleration

           

       Also the angular velocity defines the speed with which a body moves around a fixed axis and this mathematically defined as

             w =\frac{\Delta \theta}{\Delta t}

          w_f = w_{in} + \alpha t

where  w_f is final angular velocity and

     => w_f = 0.25 +(0.891)(0.194)

               =0.43\ rev /s

 Now the angular displacement(\theta) is the angle made by a body moving in a circular path and it show us the relationship between the distance moved around the circular path and the distance move at the center of the circular path in terms of angle and this is measured in radians

 The angular displacement can also be expressed as

                 \theta = w_{in} t + \frac{1}{2}   \alpha t^2

                    = (0.250)(0.194)+\frac{1}{2}(0.891)(0.194)^2

                \theta = 0.0652\ rev

                       

Angular acceleration is the change of angular velocity with time and this is mathematically defined as

             \alpha  =\frac{\Delta w}{\Delta t}

The tangential velocity is the velocity that is been measured at an point tangent to the circular path of motion and this mathematically represented as

             v_t = w_fr = (\frac{d}{2} )w_f

                            = \frac{0.800}{2} (0.423)

                           = [\frac{0.800}{2} ] (0.423)[\frac{2 \pi \ rad}{1.0 rev} ]

                          = 1.06 m/s

In this motion described in the problem statement we would have two acceleration component which are centripetal acceleration(a_c) and tangential acceleration (a_t)

The centripetal acceleration is defined as the rate of change of the tangential velocity and this is mathematically represented as

                 a_c = \frac{v^2}{r}

                     = \frac{(1.063 m/s)^2}{{\frac{0.800m}{2} }}

                     =2.83 \ m/s^2

this is always directed toward the center of the circular path

The tangential acceleration can be defined as the linear acceleration of the body at any point on the circular path of motion and it is mathematically

represented as

                   a_t = \alpha r

                       = [\frac{0.800m}{2} ](0.891 rev /s^2 )

                       = [\frac{0.800m}{2} ](0.891 rev/s^2)[\frac{2\pi\ rad}{1.0 rev} ]

                  a_t = 2.24 m/s^2

This directed tangential to the circular path  

Note: As shown in the diagram the two component of the acceleration are always perpendicular to each other.

Between this two component of acceleration is the resultant acceleration and it is mathematically represented as

                a_r = \sqrt{(a_c^2 + a_t^2)}

                a_r = \sqrt{(2.83m/s^2)^2 + (2.24m/s^2)^2 }

                    = 3.6 m/s^2

                   

     

   

       

 

       

           

6 0
3 years ago
Starting from the results of Examples 5.4 and 5.5, estimate the number of cubic meters of water that would flow each second thro
alexira [117]

Answer: Hello Results of examples 5.4 and 5.5 are missing from your question but I was able to find it online and use it to resolve your question

answer :

a) 1780 m^3/sec

b)  23.81 m

Explanation:

<u>a) calculate the number of m^3 of water flowing through an OTEC plant charge </u>

<em>assumption : assuming an ideal heat engine</em>

 Q / t   =  m*c*∆T * (eff) / t

1e^9 J/s = 1g/cc *V(1cal/g°C) * 2°C (6.7%)*(4.184J/cal) / t

Hence:  V / t ( number of m^3 of water ) = 1.78e^9 cc / sec = 1.78 * 10

= 1780 m^3/sec

<em><u>b) Determine the diameter of pipes </u></em>

Given that the water flows at  4m/s  ( velocity )

1780 m^3 /sec = A * V  ------ ( 1 )

A = π*d^2/4 =  1780 / 4 = 445 m^2  -------- ( 2 )

v = 4 m/s

Back to equation 2

d^2 = ( 445 * 4 ) / π

      ≈ 567

∴ necessary diameter ( d ) = \sqrt{567} = 23.81 m

3 0
2 years ago
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