GRADE 8 PRACTICE
Physics Problems: Heat engines, Grade 8
Gas operation, engine design and efficiency.
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 #22
Work done by gas and how engines workWhat concept does the description correspond to: “Gas performs mechanical work when it expands and moves the piston or turbine blades.»?
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- \text{Description}
- \text{Gas performs mechanical work when it expands and moves the piston or turbine blades.}
\text{name concepts} - ?
- \text{Let's compare approval with definition}
Some of the internal energy of the gas is converted into mechanical energy, and compression by an external force can increase the internal energy.
- \text{Let's formulate conclusion}\text{Concept} = \text{Work done by an expanding gas}
Answer\text{Concept} = \text{Work done by an expanding gas}
Problem #23
Work done by gas and how engines workWhat concept does the description correspond to: “A heat engine in which fuel is burned inside a cylinder and the expanding gas acts on a piston.»?
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- \text{Description}
- \text{A heat engine in which fuel is burned inside a cylinder and the expanding gas acts on a piston.}
\text{name concepts} - ?
- \text{Let's compare approval with definition}
The four-stroke cycle comprises intake, compression, power and exhaust. Useful work is produced mainly during the power stroke.
- \text{Let's formulate conclusion}\text{Concept} = \text{Internal combustion engine}
Answer\text{Concept} = \text{Internal combustion engine}
Problem #24
Heat enginesDuring which stroke of a four-stroke engine do heated gases directly perform useful work on the piston?
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- \text{cycle}
- \text{four tact}
\text{beat useful work} - ?
- \text{After ignition Gas pressure sharply growing}
- \text{gas expanding and pushes piston}\text{worker move}
Answer\text{worker move}
Problem #25
Heat engine efficiency and the environmentWhat concept does the description correspond to: “A device that operates in cycles, receiving heat from a hot reservoir, doing work and rejecting some energy to a cold reservoir.»?
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- \text{Description}
- \text{A device that operates in cycles, receiving heat from a hot reservoir, doing work and rejecting some energy to a cold reservoir.}
\text{name concepts} - ?
- \text{Let's compare approval with definition}
It is impossible to convert all the heat received into work, so the efficiency of any real heat engine is less than one.
- \text{Let's formulate conclusion}\text{Concept} = \text{Heat engine}
Answer\text{Concept} = \text{Heat engine}
Problem #26
Heat engine efficiency and the environmentWhat concept does the description correspond to: “The ratio of net work produced by a heat engine per cycle to heat supplied to its working substance by the hot reservoir during the same cycle.»?
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- \text{Description}
- \text{The ratio of net work produced by a heat engine per cycle to heat supplied to its working substance by the hot reservoir during the same cycle.}
\text{name concepts} - ?
- \text{Let's compare approval with definition}
For the engine, η = A/Q₁. Heat Q₁ reaching the working substance may be less than the energy qm released by fuel. For the whole installation evaluated against fuel input, use A/(qm), including heat-transfer losses. Do not mix these calculation boundaries.
- \text{Let's formulate conclusion}\text{Concept} = \text{Heat engine efficiency}
Answer\text{Concept} = \text{Heat engine efficiency}
Problem #27
Heat enginesThe engine received 400 kJ from the fuel and performed 120 kJ of useful work. Find the efficiency.
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- A
- 120\,\text{кДж}
- Q_1
- 400\,\text{кДж}
\eta - ?
- \eta=\frac{A}{Q_1}\eta=\frac{120}{400}\eta = 0{,}3
- \eta=30\,\%
Answer30\,\%
Problem #115
Work done by gas and how engines workGas 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 #116
Work done by gas and how engines workGas 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 #117
Work done by gas and how engines workGas 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 #118
Work done by gas and how engines workGas 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 #119
Work done by gas and how engines workGot 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 #120
Work done by gas and how engines workGot 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 #121
Heat engine efficiency and the environmentUseful 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 #122
Heat engine efficiency and the environmentUseful 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 #123
Heat engine efficiency and the environmentInstallation 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 #124
Heat engine efficiency and the environmentInstallation 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 #125
Heat engine efficiency and the environmentInstallation 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 #126
Heat engine efficiency and the environmentInstallation 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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