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olya-2409 [2.1K]
3 years ago
8

The heating element of a coffeemaker operates at 120 V and carries a current of 2.00 A. Assuming that the water absorbs all of t

he energy converted by the resistor, calculate how long it takes to heat 0.500 kg of water from room temperature (23.0°C) to the boiling point. (The specific heat of water is C= 4186 J/Kg oC. The energy required to bring the water to the boiling point is Q = m C ΔT.)
Physics
1 answer:
gogolik [260]3 years ago
5 0

Answer:

t=671.5s.

Explanation:

The heat needed will be provided by the power dissipated by the resistor. This power gives certain energy per unit time, so we multiply it by time to get the energy provided: Q=Pt.

The equation of heat given mass, specific heat and temperature change is Q=mC\Delta T, and the equation of power dissipated by a resistor is P=Vi.

Putting all together:

mC\Delta T=Vit.

Which means:

t=\frac{mC\Delta T}{Vi}.

From 23.0°C to 100°C we have a \Delta T=77^{\circ}C, which we won't need to put in Kelvin in this case since it is a variation, so for our values we have:

t=\frac{(0.5kg)(4186J/kg^{\circ}C)(77^{\circ}C)}{(120V)(2A)}=671.5s.

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A 100​-lb load hangs from three cables of equal length that are anchored at the points ​(minus4​,0,0), ​(2​,2 StartRoot 3 EndRoo
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Answer:

  • \vec{F}_{cable_1} =  (-19.245 \ lbf ,0, 33.333 \ lbf)
  • \vec{F}_{cable_2} =  (9.622 \ lbf , 13.608 \ lbf ,33.333 \ lbf)
  • \vec{F}_{cable_3} =  (9.622 \ lbf , -13.608 \ lbf ,33.333 \ lbf)

Explanation:

The mass of the load is

m_{load} = 100 \ lb

As the mass hangs, the cables must be tight, so, we can obtain the vector parallel to the cable as:

\vec{r}_{cable} = \vec{r}_{anchored} - \vec{r}_{load}

where \vec{r}_{load} is the position of the load and \vec{r}_{anchored}  is the point where the cable is anchored.

So, for our cables

\vec{r}_{cable_1} = (-4,0,0) - (0,0,-4\sqrt{3})=(-4,0,4\sqrt{3})

\vec{r}_{cable_2} = (2,2\sqrt{3},0) - (0,0,-4\sqrt{3})=(2,2\sqrt{2},4\sqrt{3})

\vec{r}_{cable_3} = (2,-2\sqrt{3},0) - (0,0,-4\sqrt{3})=(2,-2\sqrt{2},4\sqrt{3})

We know that the forces must be in this directions, so we can write

\vec{F}_i=k_i \vec{r}_{cable_i}

We also know, as the system is in equilibrium, the sum of the forces must be zero:

\vec{F}_{cable_1}+\vec{F}_{cable_2}+\vec{F}_{cable_3}+\vec{W}=0

where \vec{W} is the weight,

\vec{W} = (0,0,-100 \ lbf)

So, we get:

k_1 (-4,0,4\sqrt{3})  + k_2 (2,2\sqrt{2},4\sqrt{3}) + k_3 (2,-2\sqrt{2},4\sqrt{3}) + (0,0,-100 \ lbf) = (0,0,0)

This gives us the following equations:

  1. -4 \ k_1 + 2 \ k_2 + 2 \ k_3  = 0
  2. 2\sqrt{2} \ k_2  -2\sqrt{2} \ k_3 = 0
  3. 4\sqrt{3} \ k_1   +  4\sqrt{3}  \ k_2 +  4\sqrt{3} \ k_3  -100 \ lbf = 0

From equation [2] is clear that k_2 = k_3, we can see that

2\sqrt{2} \ k_2  = 2\sqrt{2} \ k_3

\frac{2\sqrt{2} \ k_2}{2\sqrt{2} }  = \frac{2\sqrt{2} \ k_3}{2\sqrt{2} }

k_2 = k_3

Now, putting this in equation [1]

-4 \ k_1 + 2 \ k_2 + 2 \ k_3  = -4 \ k_1 + 2 \ k_3 + 2 \ k_3 =  -4 \ k_1 + 4 \ k_3  = 0

4 \ k_1 = 4 \ k_3

\ k_1 = \ k_3

Taking this result to the equation [3]

4\sqrt{3} \ k_1   +  4\sqrt{3}  \ k_2 +  4\sqrt{3} \ k_3  -100 \ lbf = 0

4\sqrt{3}  \ k_3   +  4\sqrt{3}  \ k_3 +  4\sqrt{3} \ k_3  = 100 \ lbf

3 * (4\sqrt{3}  \ k_3)  = 100 \ lbf

k_3  = \frac{100 \ lbf}{  12 \sqrt{3}}

k_1 = k_2 = k_3  =  \frac{100 \ lbf}{  12 \sqrt{3}}

So, the forces are:

\vec{F}_{cable_1} = k_1 (-4,0,4\sqrt{3})

\vec{F}_{cable_1} = \frac{100 \ lbf}{  12 \sqrt{3}} (-4,0,4\sqrt{3})

\vec{F}_{cable_1} =  (-\frac{100 \ lbf}{  3 \sqrt{3}},0,\frac{100 \ lbf}{3})

\vec{F}_{cable_1} =  (-19.245 \ lbf ,0, 33.333 \ lbf)

\vec{F}_{cable_2} = k_2 (2,2\sqrt{2},4\sqrt{3})

\vec{F}_{cable_2} = \frac{100 \ lbf}{  12 \sqrt{3}} (2,2\sqrt{2},4\sqrt{3})

\vec{F}_{cable_2} =  (9.622 \ lbf , 13.608 \ lbf ,33.333 \ lbf)

\vec{F}_{cable_3} = k_3 (2,-2\sqrt{2},4\sqrt{3})

\vec{F}_{cable_3} = \frac{100 \ lbf}{  12 \sqrt{3}} (2,-2\sqrt{2},4\sqrt{3})

\vec{F}_{cable_3} =  (9.622 \ lbf , -13.608 \ lbf ,33.333 \ lbf)

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