A planet orbits a star in an elliptical orbit as shown.
At which point in its orbit is the planet's kinetic energy increasing?
- \(W\)
- \(X\)
- \(Y\)
- \(Z\)
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A planet orbits a star in an elliptical orbit as shown.
At which point in its orbit is the planet's kinetic energy increasing?
\(D\)
\(\Rightarrow D\)
In a thought experiment, a projectile is launched vertically from Earth's surface. Its initial velocity is less than the escape velocity. The behaviour of the projectile can be analysed by using two different models, Model \(A\) and Model \(B\) as shown. The effects of Earth's atmosphere and Earth's rotational and orbital motions can be ignored. Compare the maximum height reached by the projectile, using each model. In your answer, describe the energy changes of the projectile. (4 marks) --- 8 WORK AREA LINES (style=lined) ---
The diagram shows two identical satellites, \(A\) and \(B\), orbiting a planet.
Which row in the table correctly compares the potential energy, \(U\), and kinetic energy, \(K\), of the satellites?
\begin{align*}
\begin{array}{l}
\ \rule{0pt}{2.5ex} \textbf{} \rule[-1.5ex]{0pt}{0pt} & \\
\rule{0pt}{2.5ex} \textbf{A.} \rule[-1ex]{0pt}{0pt} \\
\rule{0pt}{2.5ex} \textbf{B.} \rule[-1ex]{0pt}{0pt} \\
\rule{0pt}{2.5ex} \textbf{C.} \rule[-1ex]{0pt}{0pt} \\
\rule{0pt}{2.5ex} \textbf{D.} \rule[-1ex]{0pt}{0pt} \\
\end{array}
\begin{array}{|c|c|}
\hline
\rule{0pt}{2.5ex} \textit{Potential energy} \rule[-1ex]{0pt}{0pt} & \textit{Kinetic energy} \\
\hline
\rule{0pt}{2.5ex} U_\text{A} > U_\text{B} \rule[-1ex]{0pt}{0pt} & K_\text{A} < K_\text{B} \\
\hline
\rule{0pt}{2.5ex} U_\text{A} < U_\text{B} \rule[-1ex]{0pt}{0pt} & K_\text{A} > K_\text{B} \\
\hline
\rule{0pt}{2.5ex} U_\text{A} > U_\text{B} \rule[-1ex]{0pt}{0pt} & K_\text{A} > K_\text{B} \\
\hline
\rule{0pt}{2.5ex} U_\text{A} < U_\text{B} \rule[-1ex]{0pt}{0pt} & K_\text{A} < K_\text{B} \\
\hline
\end{array}
\end{align*}
\(A\)
\(\Rightarrow A\)
The International Space Station (ISS) is travelling around Earth in a stable circular orbit, as shown in the diagram below.
Which one of the following statements concerning the momentum and the kinetic energy of the ISS is correct?
\(D\)
\(\Rightarrow D\)
A 400 kg satellite is travelling in a circular orbit of radius 6.700 × 10\(^6\) m around Earth. Its potential energy is –2.389 × 10\(^{10}\ \text{J}\) and its total energy is –1.195 × 10\(^{10}\ \text{J}\). At point \(P\), the satellite's engines are fired, increasing the satellite's velocity in the direction of travel and causing its kinetic energy to increase by 5.232 × 10\(^8\ \text{J}\). Assume that this happens instantaneously and that the engine is then shut down. The satellite follows the trajectory shown, which passes through \(Q\), 6.850 × 10\(^6\) m from Earth's centre. --- 5 WORK AREA LINES (style=lined) --- --- 5 WORK AREA LINES (style=lined) --- --- 5 WORK AREA LINES (style=lined) --- a. Energy changes from \(P\) to \(Q\): b. Using the Law of Conservation of Energy: c. The orbital velocity at \(Q\) is: a. Energy changes from \(P\) to \(Q\): b. Using the Law of Conservation of Energy: c. The orbital velocity at \(Q\) is:
\(E_Q\)
\(=U_Q+K_Q\)
\(=E_P+K_{\text{engine}}\)
\(U_Q\)
\(=-\dfrac{GMm}{r}\)
\(=-\dfrac{6.67 \times 10^{-11} \times 6 \times 10^{24} \times 400}{6.85 \times 10^6}\)
\(=-2.337 \times 10^{10}\) \(\text{J}\)
\(K_Q\)
\(=E_P+K_{\text{engine}}-U_Q\)
\(=-1.195 \times 10^{10} + 5.232 \times 10^8 -(-2.337 \times 10^{10})\)
\(=1.194 \times 10^{10}\) \(\text{J … as required}\)
\(v\)
\(=\sqrt{\dfrac{GM}{r}}\)
\(=\sqrt{\dfrac{6.67 \times 10^{-11} \times 6 \times 10^{24}}{6.85 \times 10^6}}\)
\(=7.644 \times 10^3\ \text{ms}^{-1}\)
\(K_Q\)
\(=\dfrac{1}{2}mv_Q^2\)
\(v_Q\)
\(=\sqrt{\dfrac{2K_Q}{m}}\)
\(=\sqrt{\dfrac{2 \times 1.194 \times 10^{10}}{400}}\)
\(=7.727 \times 10^3\ \text{ms}^{-1}\)
\(E_Q\)
\(=U_Q+K_Q\)
\(=E_P+K_{\text{engine}}\)
\(U_Q\)
\(=-\dfrac{GMm}{r}\)
\(=-\dfrac{6.67 \times 10^{-11} \times 6 \times 10^{24} \times 400}{6.85 \times 10^6}\)
\(=-2.337 \times 10^{10}\) \(\text{J}\)
\(K_Q\)
\(=E_P+K_{\text{engine}}-U_Q\)
\(=-1.195 \times 10^{10} + 5.232 \times 10^8 -(-2.337 \times 10^{10})\)
\(=1.194 \times 10^{10}\) \(\text{J … as required}\)
\(v\)
\(=\sqrt{\dfrac{GM}{r}}\)
\(=\sqrt{\dfrac{6.67 \times 10^{-11} \times 6 \times 10^{24}}{6.85 \times 10^6}}\)
\(=7.644 \times 10^3\ \text{ms}^{-1}\)
\(K_Q\)
\(=\dfrac{1}{2}mv_Q^2\)
\(v_Q\)
\(=\sqrt{\dfrac{2K_Q}{m}}\)
\(=\sqrt{\dfrac{2 \times 1.194 \times 10^{10}}{400}}\)
\(=7.727 \times 10^3\ \text{ms}^{-1}\)
A bullet is fired vertically from the surface of Mars, at the escape velocity of Mars. Another bullet is fired vertically from the surface of Earth, at the escape velocity of Earth.
Neglecting air resistance, compare the energy transformations of the two bullets. (5 marks)
A rocket carrying a satellite is launched from Earth. Once the rocket engine is switched off the satellite continues in an elliptical orbit.
Explain the satellite's changes in energy during this journey. (3 marks)
The following makeshift device was made to provide lighting for a stranded astronaut on Mars.
The mass of Mars is `6.39 ×10^(23) \ text {kg}`.
The 2 kg mass falls, turning the DC generator, which supplies energy to the light bulb. The mass falls from a point that is 3 376 204 m from the centre of Mars.
--- 8 WORK AREA LINES (style=lined) ---
--- 8 WORK AREA LINES (style=lined) ---
a. 7.48 J
b. When switch is opened:
a. `DeltaE=U_(f)-U_(i)`
`=((-Gm_(1)m_(2))/(r_(f)))-((-Gm_(1)m_(2))/(r_(i)))`
`=(-6.67 xx10^(-11)xx6.39 xx10^(23)xx2)/(3\ 376\ 203)-((-6.67 xx10^(-11)xx6.39 xx10^(23)xx2))/(3\ 376\ 204)`
`=-7.48\ text{J}`
b. When switch is opened:
The escape velocity from a planet is given by `v = sqrt((2GM)/(r))`.
--- 4 WORK AREA LINES (style=lined) ---
--- 6 WORK AREA LINES (style=lined) ---
a. `v=5010 text{m s}^(-1)`
b. Applying the law of conservation of energy:
| `KE_(i)+U_(i)` | `=0` | |
| `(1)/(2)mv^(2)-(GMm)/(r)` | `=0` | |
| `mv^(2)` | `=(2GMm)/(r)` | |
| `∴ v_(esc)` | `=sqrt((2GM)/(r))` |
| a. | `v` | `=sqrt((2xx6.67 xx10^(-11)xx6.39 xx10^(23))/(3.39 xx10^(6)))` |
| `=5014.5 text{m s}^(-1)` | ||
| `=5015 text{m s}^(-1)\ \ text{(to 0 d.p.)}` |
b. Applying the law of conservation of energy:
| `KE_(i)+U_(i)` | `=0` | |
| `(1)/(2)mv^(2)-(GMm)/(r)` | `=0` | |
| `mv^(2)` | `=(2GMm)/(r)` | |
| `∴ v_(esc)` | `=sqrt((2GM)/(r))` |
A satellite orbits Earth with an elliptical orbit that passes through positions `X` and `Y`.
Which row of the table correctly identifies the position at which the satellite has greater kinetic energy and the position at which it has greater potential energy?
\begin{align*}
\begin{array}{l}
\rule{0pt}{2.5ex}\textit{} & \textit{} \\
\textit{}\rule[-1ex]{0pt}{0pt}& \textit{} \\
\rule{0pt}{2.5ex}\textbf{A.}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{B.}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{C.}\rule[-1ex]{0pt}{0pt}\\
\rule{0pt}{2.5ex}\textbf{D.}\rule[-1ex]{0pt}{0pt}\\
\end{array}
\begin{array}{|c|c|}
\hline
\rule{0pt}{2.5ex}\textit{Greater} & \textit{Greater} \\
\quad \textit{kinetic energy}\quad \rule[-1ex]{0pt}{0pt}& \quad \textit{potential energy} \quad \\
\hline
\rule{0pt}{2.5ex}X\rule[-1ex]{0pt}{0pt}&X\\
\hline
\rule{0pt}{2.5ex}X\rule[-1ex]{0pt}{0pt}& Y\\
\hline
\rule{0pt}{2.5ex}Y\rule[-1ex]{0pt}{0pt}& X \\
\hline
\rule{0pt}{2.5ex}Y\rule[-1ex]{0pt}{0pt}& Y \\
\hline
\end{array}
\end{align*}
`B`
`=>B`
The radius of the moon is 1740 km. The moon's mass is `7.35 × 10^(22)` kg. In this question, ignore the moon's rotational and orbital motion.
A 20 kg mass is launched vertically from the moon's surface at a velocity of `1200 \ text{m s}^(-1)`.
--- 5 WORK AREA LINES (style=lined) ---
--- 10 WORK AREA LINES (style=lined) ---
a. Proof (See Worked Solutions)
b. `424 text{m s}^-1`
| a. | `U_(i)` | `=-(GMm)/(r)` |
| `=(-6.67 xx10^(-11)xx7.35 xx10^(22)xx20)/(1.74 xx10^(6))` | ||
| `=-5.64 xx10^(7)\ text{J}` | ||
| `U_(f)` | `=(-6.67 xx10^(-11)xx7.35 xx10^(22)xx20)/(2.24 xx10^(6))` | |
| `=-4.38 xx10^(7)\ text{J}` |
`:.Delta U=U_(f)-U_(i)=1.26 xx10^(7)\ text{J}`
b. `KE_(i)=(1)/(2)m u^(2)=(1)/(2)xx20 xx1200^(2)=1.44 xx10^(7) text{J}`
`KE_(f)=KE_(i)-DeltaE_(p)\ \ text{(by LCE)}=1.44 xx10^(7)-1.26 xx10^(7)=1.8 xx10^(6) text{J}`
| `(1)/(2)mv^(2)` | `=1.8 xx10^(6)` | |
| `v^2` | `=(2xx1.8 xx10^(6))/(20)` | |
| `:.v` | `=sqrt((2xx1.8 xx10^(6))/(20))= 424 text{m s}^-1` |
A rocket is launched vertically from a planet of mass \(M\). After it leaves the atmosphere, the rocket's engine is turned off and it continues to move away from the planet. From this time the rocket's mass is 200 kg. The rocket's speed, \(v\), at two different distances from the planet's centre, \(R\), is shown.
\begin{array}{|c|c|c|}
\hline \rule{0pt}{2.5ex} \text {Point } \rule[-1ex]{0pt}{0pt}& R\ \text{(m)} & \quad v\left(\text{m s}^{-1}\right) \quad \\
\hline \rule{0pt}{2.5ex} 1 \rule[-1ex]{0pt}{0pt}& \quad 4.3 \times 10^6 \quad & 5500 \\
\hline \rule{0pt}{2.5ex} 2 \rule[-1ex]{0pt}{0pt}& 2.5 \times 10^7 & 2900 \\
\hline
\end{array}
Show that the magnitude of the change in kinetic energy from point 1 to point 2 is \(2.2 \times 10^9 \ \text{J}\). (2 marks)
--- 4 WORK AREA LINES (style=lined) ---
Determine the mass \(M\) of the planet using the law of conservation of energy. (3 marks)
--- 6 WORK AREA LINES (style=lined) ---
a. \(\Delta K=K_f-K_i\)
\(K_f=\dfrac{1}{2} m v_2^2=\dfrac{1}{2} 200 \times 2900^2=8.41 \times 10^8 \ \text{J}\)
\(K_i=\dfrac{1}{2} m v_1^2=\dfrac{1}{2} 200 \times 5500^2=3.025 \times 10^9 \ \text{J}\)
| \(\therefore \Delta K\) | \(=8.41 \times 10^8-3.025 \times 10^9\) | |
| \(=-2.2 \times 10^9 \ \text{J}\) |
\(\therefore\) This change has a magnitude of \(2.2 \times 10^9 \ \text{J}\).
b. Applying the law of conservation of energy:
\(\left(2.2 \times 10^9\right)=-\dfrac{\left(6.67 \times 10^{-11}\right)(200) M}{2.5 \times 10^7}+\dfrac{\left(6.67 \times 10^{-11}\right)(200) M}{4.3 \times 10^6}\)
\(\left(2.2 \times 10^9\right)\left(2.5 \times 10^7\right)\left(4.3 \times 10^6\right)\)
\(=\left(6.67 \times 10^{-11}\right) 200 M\left[\left(2.5 \times 10^7\right)-\left(4.3 \times 10^7\right)\right]\)
| \(\therefore M\) | \(=\dfrac{\left(2.2 \times 10^9\right)\left(2.5 \times 10^7\right)\left(4.3 \times 10^6\right)}{200\left(6.67 \times 10^{-11}\right)\left[\left(2.5 \times 10^7\right)-\left(4.3 \times 10^6\right)\right]}\) | |
| \(=8.56 \times 10^{23} \ \text{kg}\) |
a. \(\Delta K=K_f-K_i\)
\(K_f=\dfrac{1}{2} m v_2^2=\dfrac{1}{2} 200 \times 2900^2=8.41 \times 10^8 \ \text{J}\)
\(K_i=\dfrac{1}{2} m v_1^2=\dfrac{1}{2} 200 \times 5500^2=3.025 \times 10^9 \ \text{J}\)
| \(\therefore \Delta K\) | \(=8.41 \times 10^8-3.025 \times 10^9\) | |
| \(=-2.2 \times 10^9 \ \text{J}\) |
\(\therefore\) This change has a magnitude of \(2.2 \times 10^9 \ \text{J}\).
b. Applying the law of conservation of energy:
\(\left(2.2 \times 10^9\right)=-\dfrac{\left(6.67 \times 10^{-11}\right)(200) M}{2.5 \times 10^7}+\dfrac{\left(6.67 \times 10^{-11}\right)(200) M}{4.3 \times 10^6}\)
\(\left(2.2 \times 10^9\right)\left(2.5 \times 10^7\right)\left(4.3 \times 10^6\right)\)
\(=\left(6.67 \times 10^{-11}\right) 200 M\left[\left(2.5 \times 10^7\right)-\left(4.3 \times 10^7\right)\right]\)
| \(\therefore M\) | \(=\dfrac{\left(2.2 \times 10^9\right)\left(2.5 \times 10^7\right)\left(4.3 \times 10^6\right)}{200\left(6.67 \times 10^{-11}\right)\left[\left(2.5 \times 10^7\right)-\left(4.3 \times 10^6\right)\right]}\) | |
| \(=8.56 \times 10^{23} \ \text{kg}\) |
The elliptical orbit of a planet around a star is shown.
Which type of energy is greater at position `P` than at `Q` ?
`A`
As the planet moves from `Q` to `P` is converted to kinetic energy.
`=>A`
A satellite is launched from the surface of Mars into an orbit that keeps it directly above a position on the surface of Mars.
Mass of Mars = `6.39 xx 10^(23)` kg
Length of Martian day = 24 hours and 40 minutes
--- 3 WORK AREA LINES (style=lined) ---
--- 6 WORK AREA LINES (style=lined) ---
a. The kinetic energy and gravitational potential energy of the satellite both increase as it moves into orbit.
b. `2.0 xx10^(7)\ \text{m}`
a. The kinetic energy and gravitational potential energy of the satellite both increase as it moves into orbit.
| b. `(r^(3))/(T^(2))` | `=(GM)/(4pi^(2))` | |
| `r^(3)` | `=((6.67 xx10^(-11)xx6.39 xx10^(23))/(4pi^(2)))((24+(40)/(60))xx60 xx60)^(2)` | |
| `:. r` | `=2.0 xx10^(7)\ \text{m}` |
A mass, `M`, is positioned at an equal distance from two identical stars as shown.
The mass is then moved to position `X`.
Which graph best represents the gravitational potential energy, `U`, of the mass during this movement?
`C`
Potential energy decreases as the mass moves closer to the stars and then increases as it moves away from them.
`=>C`