GRADE 10 PRACTICE
Physics Problems: Thermodynamics, Grade 10
Internal energy, heat, work and cycles.
Here the conditions and analysis of the solution can be read without an account. In the simulator, you need to collect the same analyzes yourself: “Given,” formulas, order of steps and answer.
Problem statements
The answer options are there to check against, and the walkthrough opens under each problem.
Problem #3
Thermodynamics: internal energy and heat transfer2\,\text{кг} ice taken from 0\,^{\circ}\text{C}, you need to melt it and heat the resulting water to 15\,^{\circ}\text{C}. How much heat will be required? Assume the specific heat of fusion of ice is 330 kJ/kg and the specific heat capacity of water is 4200 J/(kg K).
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- m
- 2\,\text{кг}
- t_1
- 0\,^{\circ}\text{C}
- t_2
- 15\,^{\circ}\text{C}
- \lambda
- 330\,000\,\tfrac{\text{Дж}}{\text{кг}}
- c
- 4200\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
Q - ?
- Q = Q_1 + Q_2 = m\lambda + mc\left(t_2 - t_1\right)
First the ice melts, then the resulting water is heated.
- Q_1 = m\lambdaQ_1 = 2\,\text{кг}\cdot 330\,000\,\tfrac{\text{Дж}}{\text{кг}}Q_1 = 660\,000\,\text{Дж}
- Q_2 = mc\left(t_2 - t_1\right)Q_2 = 2\,\text{кг}\cdot 4200\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}\cdot 15\,^{\circ}\text{C}Q_2 = 126\,000\,\text{Дж}
- Q = Q_1 + Q_2Q = 660\,000\,\text{Дж} + 126\,000\,\text{Дж}Q = 786\,000\,\text{Дж}
AnswerQ = 786\,000\,\text{Дж}
Problem #82
Thermodynamics: internal energy and heat transferHow much heat is required to 2\,\text{кг} ice at -40\,^{\circ}\text{C} turn into water vapor 100\,^{\circ}\text{C}? Take the heat capacities of ice and water as 2100 and 4200 J/(kg K), the specific heat of melting of ice as 330 kJ/kg and the heat of vaporization of water as 2.3 MJ/kg.
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- m
- 2\,\text{кг}
- t_1
- -40\,^{\circ}\text{C}
- t_2
- 0\,^{\circ}\text{C}
- t_3
- 100\,^{\circ}\text{C}
- c_1
- 2100\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- \lambda
- 330\,000\,\tfrac{\text{Дж}}{\text{кг}}
- c_2
- 4200\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- r
- 2\,300\,000\,\tfrac{\text{Дж}}{\text{кг}}
Q - ?
- Q = mc_1\left(t_2 - t_1\right) + m\lambda + mc_2\left(t_3 - t_2\right) + mr
Four stages: heating ice, melting, heating water, evaporation.
- Q = 2\cdot 2100\cdot 40 + 2\cdot 330\,000 + 2\cdot 4200\cdot 100 + 2\cdot 2\,300\,000Q = 168\,000 + 660\,000 + 840\,000 + 4\,600\,000Q = 6\,268\,000\,\text{Дж}
AnswerQ = 6\,268\,000\,\text{Дж}
Problem #83
Thermodynamics: internal energy and heat transferDefine internal energy 20\,\text{г} helium at 7\,^{\circ}\text{C}.
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- m
- 20\,\text{г}
- t
- 7\,^{\circ}\text{C}=T = 280\,\text{К}
- M
- 4\,\tfrac{\text{г}}{\text{моль}}
- R
- 8{,}31\,\tfrac{\text{Дж}}{\text{К}\cdot\text{моль}}
U - ?
- U = \dfrac{3}{2}\cdot\dfrac{m}{M}RT
Helium is monatomic, so there are three degrees of freedom per molecule.
- U = \dfrac{3mRT}{2M}U = \dfrac{3\cdot 20\cdot 8{,}31\cdot 280}{2\cdot 4}U = 17\,451\,\text{Дж}
AnswerU = 17\,451\,\text{Дж}
Problem #84
Thermodynamics: internal energy and heat transferHow much alcohol do you need to burn to melt? 3\,\text{кг} lead taken from 127\,^{\circ}\text{C}? The melting point of lead is 327 °C, its specific heat capacity is 130 J/(kg K), the specific heat of fusion is 25 kJ/kg. The specific heat of combustion of alcohol is 29 MJ/kg. All the heat of combustion is transferred to lead.
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- m
- 3\,\text{кг}
- t_1
- 127\,^{\circ}\text{C}
- t_2
- 327\,^{\circ}\text{C}
- c
- 130\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- \lambda
- 25\,000\,\tfrac{\text{Дж}}{\text{кг}}
- q
- 29\cdot 10^{6}\,\tfrac{\text{Дж}}{\text{кг}}
m_2 - ?
- Q = mc\left(t_2 - t_1\right) + m\lambda3\cdot 130\cdot 200 + 3\cdot 25\,000 = 78\,000 + 75\,000Q = 153\,000\,\text{Дж}
Lead is first heated to its melting point and then melted.
- Q = m_2 q\ \Rightarrow\ m_2 = \dfrac{Q}{q}m_2 = \dfrac{153\,000}{29\cdot 10^{6}}m_2 = 5{,}3\cdot 10^{-3}\,\text{кг} = 5{,}3\,\text{г}
Answerm_2 = 5{,}3\,\text{г}
Problem #85
Thermodynamics: heat enginesHot reservoir temperature 327\,^{\circ}\text{C}, refrigerator -33\,^{\circ}\text{C}. What is the maximum efficiency? How much heat does a reversible Carnot engine receive from the hot reservoir if the heat rejected to the cold reservoir is 300\,\text{Дж}?
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- t_1
- 327\,^{\circ}\text{C}=T_1 = 600\,\text{К}
- t_2
- -33\,^{\circ}\text{C}=T_2 = 240\,\text{К}
- Q_2
- 300\,\text{Дж}
\eta - ?Q_1 - ?
- \eta = \dfrac{T_1 - T_2}{T_1}\eta = \dfrac{600 - 240}{600}\eta = 0{,}6
The maximum efficiency is given by the Carnot cycle.
- \eta = \dfrac{Q_1 - Q_2}{Q_1}\ \Rightarrow\ Q_2 = Q_1\left(1 - \eta\right)
- Q_1 = \dfrac{Q_2}{1 - \eta}Q_1 = \dfrac{300}{1 - 0{,}6}Q_1 = 750\,\text{Дж}
Answer\eta = 0{,}6Q_1 = 750\,\text{Дж}
Problem #86
Thermodynamics: internal energy and heat transferA monatomic gas is heated isobarically at pressure 2\cdot10^{5}\,\text{Па}. Volume increased by 15\,\text{л}. Determine the work done, the change in internal energy, and the heat gained.
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- p
- 2\cdot 10^{5}\,\text{Па}
- \Delta V
- 15\,\text{л}=15\cdot 10^{-3}\,\text{м}^{3}
A - ?\Delta U - ?Q - ?
- A = p\,\Delta VA = 2\cdot 10^{5}\cdot 15\cdot 10^{-3}A = 3000\,\text{Дж}
- \Delta U = \dfrac{3}{2}\nu R\,\Delta T = \dfrac{3}{2}p\,\Delta V = \dfrac{3}{2}A\Delta U = \dfrac{3}{2}\cdot 3000\Delta U = 4500\,\text{Дж}
- Q = \Delta U + A = \dfrac{5}{2}AQ = \dfrac{5}{2}\cdot 3000Q = 7500\,\text{Дж}
In an isobaric process, work accounts for two-fifths of the heat input.
AnswerA = 3000\,\text{Дж}\Delta U = 4500\,\text{Дж}Q = 7500\,\text{Дж}
Problem #87
Thermodynamics: internal energy and heat transferThe bath is filled 80\,\text{л} water at 15\,^{\circ}\text{C}. How much water at 80\,^{\circ}\text{C} need to be added to get 40\,^{\circ}\text{C}?
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- m_1
- 80\,\text{кг}
- t_1
- 15\,^{\circ}\text{C}
- t_2
- 80\,^{\circ}\text{C}
- \theta
- 40\,^{\circ}\text{C}
V_2 - ?
- m_1 c\left(\theta - t_1\right) = m_2 c\left(t_2 - \theta\right)
Heat balance equation; the specific heat capacity decreases.
- m_2 = \dfrac{m_1\left(\theta - t_1\right)}{t_2 - \theta}m_2 = \dfrac{80\cdot 25}{40}V_2 = 50\,\text{кг} \Rightarrow V_2 = 50\,\text{л}
AnswerV_2 = 50\,\text{л}
Problem #88
Thermodynamics: internal energy and heat transferInto the water at 50\,^{\circ}\text{C} threw a piece of ice 20\,\text{г} at 0\,^{\circ}\text{C}. The temperature dropped to 20\,^{\circ}\text{C}. What is the initial mass of water? The specific heat of melting of ice is 330 kJ/kg, the heat capacity of water is 4200 J/(kg K). Neglect heat exchange with the environment.
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- t_1
- 50\,^{\circ}\text{C}
- m_2
- 20\,\text{г}=0{,}02\,\text{кг}
- t_2
- 0\,^{\circ}\text{C}
- \theta
- 20\,^{\circ}\text{C}
- c
- 4200\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- \lambda
- 330\,000\,\tfrac{\text{Дж}}{\text{кг}}
m_1 - ?
- m_1 c\left(t_1 - \theta\right) = m_2\lambda + m_2 c\left(\theta - t_2\right)
The ice first melts, then the resulting water is heated to a common temperature.
- m_1 = \dfrac{m_2\lambda + m_2 c\left(\theta - t_2\right)}{c\left(t_1 - \theta\right)}m_1 = \dfrac{0{,}02\cdot 330\,000 + 0{,}02\cdot 4200\cdot 20}{4200\cdot 30}m_1 = 0{,}0657\,\text{кг} = 65{,}7\,\text{г}
Answerm_1 = 65{,}7\,\text{г}
Problem #89
Thermodynamics: internal energy and heat transferIn a glass of mass 100\,\text{г} poured 200\,\text{г} water at 30\,^{\circ}\text{C}. How much ice at -15\,^{\circ}\text{C} must be added to cool the system to 10\,^{\circ}\text{C}? Glass glass. Specific heat capacities of glass, water and ice: 830, 4200 and 2100 J/(kg K). The specific heat of melting of ice is 330 kJ/kg. Neglect heat exchange with the environment.
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- m_1
- 0{,}1\,\text{кг}
- m_2
- 0{,}2\,\text{кг}
- t_1
- 30\,^{\circ}\text{C}
- t_3
- -15\,^{\circ}\text{C}
- t_2
- 0\,^{\circ}\text{C}
- \theta
- 10\,^{\circ}\text{C}
- c_1
- 830\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- c_2
- 4200\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- c_3
- 2100\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- \lambda
- 330\,000\,\tfrac{\text{Дж}}{\text{кг}}
m_3 - ?
- m_1 c_1\left(t_1 - \theta\right) + m_2 c_2\left(t_1 - \theta\right) = m_3\left[c_3\left(t_2 - t_3\right) + \lambda + c_2\left(\theta - t_2\right)\right]
On the left the glass and water give off heat, on the right the ice heats up, melts and heats up like water.
- m_3 = \dfrac{m_1 c_1\left(t_1 - \theta\right) + m_2 c_2\left(t_1 - \theta\right)}{c_3\left(t_2 - t_3\right) + \lambda + c_2\left(\theta - t_2\right)}m_3 = \dfrac{0{,}1\cdot 830\cdot 20 + 0{,}2\cdot 4200\cdot 20}{2100\cdot 15 + 330\,000 + 4200\cdot 10}m_3 = 4{,}6\cdot 10^{-2}\,\text{кг} = 46\,\text{г}
Answerm_3 = 46\,\text{г}
Problem #90
Thermodynamics: internal energy and heat transferMass into the water 2\,\text{кг} at 20\,^{\circ}\text{C} let me in 100\,\text{г} water vapor at 100\,^{\circ}\text{C}. What temperature will it be? The specific heat of vaporization of water is 2.3 MJ/kg, the heat capacity of water is 4200 J/(kg K). Neglect heat exchange with the environment.
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- m_1
- 2\,\text{кг}
- t_1
- 20\,^{\circ}\text{C}
- m_2
- 100\,\text{г}=0{,}1\,\text{кг}
- t_2
- 100\,^{\circ}\text{C}
- c
- 4200\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- r
- 2\,300\,000\,\tfrac{\text{Дж}}{\text{кг}}
\theta - ?
- m_1 c\left(\theta - t_1\right) = m_2 r + m_2 c\left(t_2 - \theta\right)
The steam first condenses, then the resulting water cools.
- \theta = \dfrac{m_2 r + m_2 c t_2 + m_1 c t_1}{m_1 c + m_2 c}\theta = \dfrac{0{,}1\cdot 2\,300\,000 + 0{,}1\cdot 4200\cdot 100 + 2\cdot 4200\cdot 20}{2\cdot 4200 + 0{,}1\cdot 4200}\theta = 50\,^{\circ}\text{C}
Answer\theta = 50\,^{\circ}\text{C}
Problem #91
Thermodynamics: internal energy and heat transferDetermine work during isobaric expansion 56\,\text{г} nitrogen, if the initial temperature 0\,^{\circ}\text{C}, and the volume increased by 3 times.
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- m
- 56\,\text{г}
- t_1
- 0\,^{\circ}\text{C}=T_1 = 273\,\text{К}
- V_2
- 3V_1
- M
- 28\,\tfrac{\text{г}}{\text{моль}}
- R
- 8{,}31\,\tfrac{\text{Дж}}{\text{К}\cdot\text{моль}}
A - ?
- \dfrac{V_1}{T_1} = \dfrac{V_2}{T_2}\ \Rightarrow\ T_2 = \dfrac{V_2 T_1}{V_1} = 3T_1T_2 = 3\cdot 273T_2 = 819\,\text{К}
- A = p\,\Delta V = \dfrac{m}{M}R\left(T_2 - T_1\right)A = \dfrac{56\cdot 8{,}31\cdot 546}{28}A = 9074{,}5\,\text{Дж}
AnswerA = 9074{,}5\,\text{Дж}
Problem #93
Thermodynamics: internal energy and heat transferIn a steel mug weighing 500\,\text{г} there is water at 15\,^{\circ}\text{C}. A copper cylinder with a mass of 200\,\text{г} at 150\,^{\circ}\text{C}. After heat exchange the temperature became 20\,^{\circ}\text{C}. What is the mass of water? Take the specific heat capacities of steel, water and copper equal to 500, 4200 and 400 J/(kg K). Neglect heat exchange with the environment.
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- m_1
- 500\,\text{г}=0{,}5\,\text{кг}
- t_1 = t_2
- 15\,^{\circ}\text{C}
- m_3
- 200\,\text{г}=0{,}2\,\text{кг}
- t_3
- 150\,^{\circ}\text{C}
- \theta
- 20\,^{\circ}\text{C}
- c_1
- 500\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- c_2
- 4200\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
- c_3
- 400\,\tfrac{\text{Дж}}{\text{кг}\cdot{}^{\circ}\text{C}}
m_2 - ?
- m_1 c_1\left(\theta - t_1\right) + m_2 c_2\left(\theta - t_2\right) = m_3 c_3\left(t_3 - \theta\right)
The mug and water heat up, the copper cylinder cools down.
- m_2 = \dfrac{m_3 c_3\left(t_3 - \theta\right) - m_1 c_1\left(\theta - t_1\right)}{c_2\left(\theta - t_2\right)}m_2 = \dfrac{0{,}2\cdot 400\cdot 130 - 0{,}5\cdot 500\cdot 5}{4200\cdot 5}m_2 = 0{,}44\,\text{кг}
Answerm_2 = 0{,}44\,\text{кг}
Problem #195
Internal energy and the first lawGas expands at constant pressure 100000 Pa, increasing the volume by 0{,}002 m³. Find the work done by the gas.
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- p
- 100000\,\text{Па}
- V
- 0{,}002\,\text{м}^{3}
A - ?
- A=p\Delta VA=100000 \cdot 0{,}002A=200\,\text{Дж}
During expansion, the work done by the gas is positive.
Answer200\,\text{Дж}
Problem #196
Internal energy and the first lawGas expands at constant pressure 200000 Pa, increasing the volume by 0{,}003 m³. Find the work done by the gas.
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- p
- 200000\,\text{Па}
- V
- 0{,}003\,\text{м}^{3}
A - ?
- A=p\Delta VA=200000 \cdot 0{,}003A=600\,\text{Дж}
During expansion, the work done by the gas is positive.
Answer600\,\text{Дж}
Problem #197
Internal energy and the first lawGas received 1000 J of heat and expanded from 0{,}002 up to 0{,}005 m³ at constant pressure 100000 Pa. Find the change in internal energy.
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- Q
- 1000\,\text{Дж}
- V_1
- 0{,}002\,\text{м}^{3}
- V_2
- 0{,}005\,\text{м}^{3}
- p
- 100000\,\text{Па}
\Delta U - ?
- A=p(V_2-V_1)A=100000 \cdot (0{,}005 - 0{,}002)A=300\,\text{Дж}
We find the work done by the gas itself.
- \Delta U=Q-A\Delta U=1000 - 300\Delta U=700\,\text{Дж}
The remaining energy increases internal energy.
Answer700\,\text{Дж}
Problem #198
Internal energy and the first lawGas received 1800 J of heat and expanded from 0{,}003 up to 0{,}007 m³ at constant pressure 200000 Pa. Find the change in internal energy.
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- Q
- 1800\,\text{Дж}
- V_1
- 0{,}003\,\text{м}^{3}
- V_2
- 0{,}007\,\text{м}^{3}
- p
- 200000\,\text{Па}
\Delta U - ?
- A=p(V_2-V_1)A=200000 \cdot (0{,}007 - 0{,}003)A=800\,\text{Дж}
We find the work done by the gas itself.
- \Delta U=Q-A\Delta U=1800 - 800\Delta U=1000\,\text{Дж}
The remaining energy increases internal energy.
Answer1000\,\text{Дж}
Problem #199
Internal energy and the first lawGot gas first 500 J at constant volume. Then I got more 900 J and expanded by 0{,}002 m³ at pressure 100000 Pa. Find the total change in internal energy.
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- Q_1
- 500\,\text{Дж}
- Q_2
- 900\,\text{Дж}
- V
- 0{,}002\,\text{м}^{3}
- p
- 100000\,\text{Па}
\Delta U - ?
- A=p\Delta VA=100000 \cdot 0{,}002A=200\,\text{Дж}
With a constant amount of work there is no; it arises only at the second stage.
- Q=Q_1+Q_2Q=500 + 900Q=1400\,\text{Дж}
Add up the resulting heat.
- \Delta U=Q-A\Delta U=1400 - 200\Delta U=1200\,\text{Дж}
We apply the first law to the entire process.
Answer1200\,\text{Дж}
Problem #200
Internal energy and the first lawGot gas first 800 J at constant volume. Then I got more 1200 J and expanded by 0{,}003 m³ at pressure 200000 Pa. Find the total change in internal energy.
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- Q_1
- 800\,\text{Дж}
- Q_2
- 1200\,\text{Дж}
- V
- 0{,}003\,\text{м}^{3}
- p
- 200000\,\text{Па}
\Delta U - ?
- A=p\Delta VA=200000 \cdot 0{,}003A=600\,\text{Дж}
With a constant amount of work there is no; it arises only at the second stage.
- Q=Q_1+Q_2Q=800 + 1200Q=2000\,\text{Дж}
Add up the resulting heat.
- \Delta U=Q-A\Delta U=2000 - 600\Delta U=1400\,\text{Дж}
We apply the first law to the entire process.
Answer1400\,\text{Дж}
Problem #201
Thermal processes and efficiencyUseful installation work 300 J at energy expended 500 J. Find the efficiency as a percentage.
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- A
- 300\,\text{Дж}
- Q
- 500\,\text{Дж}
\eta - ?
- \eta=\frac{A}{Q}\cdot100\eta=\frac{300}{500} \cdot 100\eta=60\,\text{\%}
Useful energy does not exceed expended energy.
Answer60\,\text{\%}
Problem #202
Thermal processes and efficiencyUseful installation work 450 J at energy expended 1000 J. Find the efficiency as a percentage.
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- A
- 450\,\text{Дж}
- Q
- 1000\,\text{Дж}
\eta - ?
- \eta=\frac{A}{Q}\cdot100\eta=\frac{450}{1000} \cdot 100\eta=45\,\text{\%}
Useful energy does not exceed expended energy.
Answer45\,\text{\%}
Problem #203
Thermal processes and efficiencyInstallation received 2000 J of energy and has efficiency 60 %. How much energy was wasted?
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- Q
- 2000\,\text{Дж}
- e
- 60\,\text{\%}
R - ?
- A=Q\frac{\eta}{100}A=\frac{2000 \cdot 60}{100}A=1200\,\text{Дж}
We convert the percentage of efficiency into a share.
- R=Q-AR=2000 - 1200R=800\,\text{Дж}
The losses account for the remaining energy.
Answer800\,\text{Дж}
Problem #204
Thermal processes and efficiencyInstallation received 3000 J of energy and has efficiency 70 %. How much energy was wasted?
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- Q
- 3000\,\text{Дж}
- e
- 70\,\text{\%}
R - ?
- A=Q\frac{\eta}{100}A=\frac{3000 \cdot 70}{100}A=2100\,\text{Дж}
We convert the percentage of efficiency into a share.
- R=Q-AR=3000 - 2100R=900\,\text{Дж}
The losses account for the remaining energy.
Answer900\,\text{Дж}
Problem #205
Thermal processes and efficiencyInstallation receives 10000 J. The first stage passes on 80 % of energy, the second turns into useful work 50 % of energy received by it. Find the total energy loss.
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- Q
- 10000\,\text{Дж}
- e_1
- 80\,\text{\%}
- e_2
- 50\,\text{\%}
R - ?
- E=Q\frac{\eta_1}{100}E=\frac{10000 \cdot 80}{100}E=8000\,\text{Дж}
In the second stage, only the energy after the first is available.
- A=E\frac{\eta_2}{100}A=\frac{8000 \cdot 50}{100}A=4000\,\text{Дж}
The efficiencies of the stages are multiplied, not added.
- R=Q-AR=10000 - 4000R=6000\,\text{Дж}
Subtract the final useful work from the initial energy.
Answer6000\,\text{Дж}
Problem #206
Thermal processes and efficiencyInstallation receives 20000 J. The first stage passes on 75 % of energy, the second turns into useful work 60 % of energy received by it. Find the total energy loss.
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- Q
- 20000\,\text{Дж}
- e_1
- 75\,\text{\%}
- e_2
- 60\,\text{\%}
R - ?
- E=Q\frac{\eta_1}{100}E=\frac{20000 \cdot 75}{100}E=15000\,\text{Дж}
In the second stage, only the energy after the first is available.
- A=E\frac{\eta_2}{100}A=\frac{15000 \cdot 60}{100}A=9000\,\text{Дж}
The efficiencies of the stages are multiplied, not added.
- R=Q-AR=20000 - 9000R=11000\,\text{Дж}
Subtract the final useful work from the initial energy.
Answer11000\,\text{Дж}
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