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WITCHER [35]
4 years ago
8

Which quantity below is a derived quantity?

Physics
2 answers:
andrew11 [14]4 years ago
7 0
C.) speed is derived quantity.
Reil [10]4 years ago
4 0

By definition, the speed of an object is given by:

v = \frac{dr}{dt}

Where,

dr/dt: derived from the position with respect to time

Therefore, speed has units of length over units of time.

Thus, speed is a derived quantity, since it depends on the value of two other quantities.

Answer:

a derived quantity is:

C. Speed

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Answer:

halved

Explanation:

the formula

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(True or False Statement)
sertanlavr [38]
False is correct......
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The force of attraction that a -40.0 μC point charge exerts on a +108 μC point charge has magnitude 4.00 N. How far apart are th
Karolina [17]

Answer:

F = k q1 q2 / r^2

r^2 = k q1 q2 / F  = 9E9 * 4E-5 * 10.8E-5 / 4

r^2 = 9 * 4 * 10.8 / 4 * E-1 = 9.72 m^2

r = 3.12 m

8 0
3 years ago
A centripetal-acceleration addict rides in uniform circular motion with period T = 2.0 s and radius r = 3.00 m. At t1 his accele
Dmitry_Shevchenko [17]

centripetal acceleration always points  towards the center of the circular path and velocity of object in circular motion always points towards the tangent on the the circle in this way centripetal acceleration and velocity are perpendicular to each other and the dot product of  perpendicular vectors is always zero,

therefore v•a=vacosα...........(1)

here α is angle between centripetal acceleration and velocity which is 90

therfore,

From equation (1)

v.a= vacos90

v.a=vax0..............(because cos90=0)

v.a=0 m^2

centripetal acceleration vector points towards center  it means it point towards inwards direction, so it lies along the radius vector,and radius vector points towards outward direction of the circle in this way centripetal acceleration and radius vector are in exact opposite direction so angle between them is 180 degree,

therefore r x a = rasin180

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6 0
3 years ago
The working substance of a certain Carnot engine is 1.90 of an ideal
Ulleksa [173]

Answer:

Explanation:

The energy for an isothermal expansion can be computed as:

\mathsf{Q_H =nRTIn (\dfrac{V_b}{V_a})} --- (1)

However, we are being told that the volume of the gas is twice itself when undergoing adiabatic expansion. This implies that:

V_b = 2V_a

Equation (1) can be written as:

\mathtt{Q_H = nRT_H In (2)}

Also, in a Carnot engine, the efficiency can be computed as:

\mathtt{e = 1 - \dfrac{T_L}{T_H}}

e = \dfrac{T_H-T_L}{T_H}

In addition to that, for any heat engine, the efficiency e =\dfrac{W}{Q_H}

relating the above two equations together, we have:

\dfrac{T_H-T_L}{T_H} = \dfrac{W}{Q_H}

Making the work done (W) the subject:

W = Q_H \Big(\dfrac{T_H-T_L}{T_H} \Big)

From equation (1):

\mathsf{W = nRT_HIn(2)  \Big(\dfrac{T_H-T_L}{T_H} \Big)}

\mathsf{W = nRIn(2)  \Big(T_H-T_L} \Big)}

If we consider the adiabatic expansion as well:

PV^y = constant

i.e.

P_bV_b^y = P_cV_c^y

From ideal gas PV = nRT

we can have:

\dfrac{nRT_H}{V_b}(V_b^y)=  \dfrac{nRT_L}{V_c}(V_c^y)

T_H =  T_L \Big(\dfrac{V_c}{V_b}\Big)^{y-1}

From the question, let us recall  aw we are being informed that:

If the volumes changes by a factor = 5.7

Then, it implies that:

\Big(\dfrac{V_c}{V_b}\Big) = 5.7

∴

T_H =  T_L (5.7)^{y-1}

In an ideal monoatomic gas \gamma = 1.6

As such:

T_H =  T_L (5.7)^{1.6-1}

T_H =  T_L (5.7)^{0.67}

Replacing the value of T_H =  T_L (5.7)^{0.67} into equation \mathsf{W = nRIn(2)  \Big(T_H-T_L} \Big)}

\mathsf{W =  nRT_L In(2) (5.7 ^{0.67 }-1}})

From in the question:

W = 930 J and the moles = 1.90

using 8.314 as constant

Then:

\mathsf{930 =  (1.90)(8.314)T_L In(2) (5.7 ^{0.67 }-1}})

\mathsf{930 = 15.7966\times 1.5315 (T_L )})

\mathsf{T_L= \dfrac{930 }{15.7966\times 1.5315}}

\mathbf{T_L \simeq = 39 \ K}

From T_H =  T_L (5.7)^{0.67}

\mathsf{T_H =  39 (5.7)^{0.67}}

\mathbf{T_H \simeq  125K}

5 0
3 years ago
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