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svlad2 [7]
3 years ago
8

A stone of mass m is thrown upward at a 30? angle to the horizontal. At the instant the stone reaches its highest point, why is

the stone neither gaining nor losing speed?
Physics
2 answers:
mash [69]3 years ago
8 0

Answer:

At highest point of the path the acceleration is perpendicular to velocity direction so there is no change in speed at this moment.

Explanation:

When an object is thrown at an angle of 30 degree with the horizontal with some initial speed

then we will have

v_i = v_ocos\theta \hat i + v_o sin\theta\hat j

now its acceleration due to gravity is given as

a = 0 - g\hat j

with the help of kinematics we can say that its velocity after any time "t" is given as

v_f = v_i + at

v_f = v_ocos\theta \hat i + (v_o sin\theta - gt)\hat j

now when it will reach to its highest point then its velocity in y direction becomes zero

v_f = v_o cos\theta \hat i

now since final velocity is along x direction only at the highest point while its acceleration at that point is due to gravity so at that moment there is no change in speed.

lora16 [44]3 years ago
6 0
First you need to know to gain or lose speed you must have acceleration of deacceleration in the direction of speed !!

so at highest point , the only acceleration is gravity and that is in the downward direction so , the velocity remains constant !!
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3 years ago
1) A thin ring made of uniformly charged insulating material has total charge Q and radius R. The ring is positioned along the x
allochka39001 [22]

Answer:

(A) considering the charge "q" evenly distributed, applying the technique of charge integration for finite charges, you obtain the expression for the potential along any point in the Z-axis:

V(z)=\frac{Q}{4\pi (\epsilon_{0}) \sqrt{R^{2} +z^{2}}  }

With (\epsilon_{0}) been the vacuum permittivity

(B) The expression for the magnitude of the E(z) electric field along the Z-axis is:

E(z)=\frac{QZ}{4\pi (\epsilon_{0}) (R^{2} +z^{2})^{\frac{3}{2} }    }

Explanation:

(A) Considering a uniform linear density λ_{0} on the ring, then:

dQ=\lambda dl (1)⇒Q=\lambda_{0} 2\pi R(2)⇒\lambda_{0}=\frac{Q}{2\pi R}(3)

Applying the technique of charge integration for finite charges:

V(z)= 4\pi (ε_{0})\int\limits^a_b {\frac{1}{ r'  }} \, dQ(4)

Been r' the distance between the charge and the observation point and a, b limits of integration of the charge. In this case a=2π and b=0.

Using cylindrical coordinates, the distance between a point of the Z-axis and a point of a ring with R radius is:

r'=\sqrt{R^{2} +Z^{2}}(5)

Using the expressions (1),(4) and (5) you obtain:

V(z)= 4\pi (\epsilon_{0})\int\limits^a_b {\frac{\lambda_{0}R}{ \sqrt{R^{2} +Z^{2}}  }} \, d\phi

Integrating results:

V(z)=\frac{Q}{4\pi (\epsilon_{0}) \sqrt{R^{2} +z^{2}}  }   (S_a)

(B) For the expression of the magnitude of the field E(z), is important to remember:

|E| =-\nabla V (6)

But in this case you only work in the z variable, soo the expression (6) can be rewritten as:

|E| =-\frac{dV(z)}{dz} (7)

Using expression (7) and (S_a), you get the expression of the magnitude of the field E(z):

E(z)=\frac{QZ}{4\pi (\epsilon_{0}) (R^{2} +z^{2})^{\frac{3}{2} }    } (S_b)

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Answer:

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