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VLD
2 months ago
6

Ability of the muscles to function effectively and efficiently without undue fatigue

Physics
1 answer:
Keith_Richards [3.2K]2 months ago
7 0

Response:

Physical well-being

Clarification:

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A container is filled with an ideal diatomic gas to a pressure and volume of P1 and V1, respectively. The gas is then warmed in
Maru [3345]

Answer:

Explanation:

The transitions occur as follows:

P₁ V₁ changes to 3P₁, V₁ (with constant volume) — first phase.

Subsequently, 3P₁,V₁ transitions to 3P₁, 5V₁ (with constant pressure) — second phase.

During the initial phase, the temperature must be escalated by a factor of 3. Therefore, if the starting temperature is T₁, then the ending temperature will be 3 T₁.

P₁V₁ = n R T₁, where n represents the number of moles of gas.

Thus, nRT₁ = P₁V₁.

The heat added at constant volume is given by n Cv (3T₁ - T₁),

= n x 5/3 R X 2T₁ (noting that for diatomic gas, Cv = 5/3 R).

= 10/3 x nRT₁

= 10/3 x P₁V₁.

In the second phase, the temperature must rise 5 times. Thus, if the initial temperature is 3T₁, then the final temperature will be 15 T₁.

The heat added at constant pressure in this scenario becomes:

= n Cp (15T₁ - 3T₁)

= n x 7/3 R X 12T₁ (for diatomic gases, Cp = 7/3 R).

= 28 x nRT₁

= 28 P₁V₁.

6 0
2 months ago
Medical cyclotrons need efficient sources of protons to inject into their center. In one kind of ion source, hydrogen atoms (i.e
Keith_Richards [3271]

Answer:

The radius is r = 4.434 *10^{-5} \ m

Explanation:

The problem states that

    The magnetic field is  B = 90 mT = 90*10^{-3} \ T

     The electron kinetic energy is  KE = 1.4 eV = 1.4 * (1.60*10^{-19}) =2.24*10^{-19} \ J

In general, for a collision to happen, the centripetal force on the electron in its orbit must equal the magnetic force acting on it  

   This can be mathematically expressed as

   \frac{mv^2}{r} = qvB

=>    r = \frac{m* v}{q * B}

Where  m denotes the electron’s mass, which has a value of m = 9.1 *10^{-31} \ kg  

             v signifies the escape velocity, mathematically represented as

                v = \sqrt{\frac{2 * KE}{m} }

Thus,

       r = \frac{m}{qB} * \sqrt{\frac{2 * KE}{m} }

     applying indices

    r = \frac{\sqrt{2 * KE * m} }{qB}

substituting these values

   

       

r = \frac{\sqrt{2 * 2.24*10^{-19}* 9.1 *10^{-31}} }{ 1.60 *10^{-19}* 90*10^{-3}}

       

r = 4.434 *10^{-5} \ m

     

6 0
23 days ago
In general, how do you find the average velocity of any object falling in a vacuum?
Softa [3030]
To determine the average velocity of an object descending in a vacuum, assuming you know its final speed, multiply the final result by the overall time. 3. The equation d = v • t expresses how distance, average velocity, and time relate to each other.
5 0
1 month ago
Two friends, Burt and Ernie, are standing at opposite ends of a uniform log that is floating in a lake. The log is 3.2m long and
Softa [3030]

Answer:

x = 0.29 m

Explanation:

It is known that the total external force acting on the mass system equals ZERO,

so the center of mass of the entire system will stay stationary.

We find that

m_1\Delta x_1 + m_2\Delta x_2 + m_3\Delta x_3 = 0

Since Ernie approaches Burt's position, we have:

33 x + 290 x + 32(-3.2 + x) = 0

355 x = 102.4

therefore, we conclude that

x = \frac{102.4}{355}

x = 0.29 m

8 0
1 month ago
15. Three semicircles of radius 1 are constructed on diameter AB of a semicircle of radius 2. The centers of the small semicircl
inna [3103]

Answer:

The area that remains is 4.201 m²

Explanation:

Provided that

AB=D=  4 m  (R=2 m)

The area of the half-circle AB is

A=\pi R^2/2

A=2π

The area of the smaller half-circle is

a=5π/6 + 2√3/4  m²

a=5π/6 + √3/2  m²

<pThus, the remaining area = A - a

                                     = 2π - (5π/6 + √3/2) m²

The remaining area is expressed as  2π - (5π/6 + √3/2) m²

5 0
1 month ago
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