Problem 82
Question
When the planet Jupiter is at a distance of \(824.7\) million \(\mathrm{km}\) from the earth, its angular diameter is measured to be \(35.72^{\prime \prime}\) of arc. The diameter of Jupiter can be calculated as (a) \(1329 \times 10^{7} \mathrm{~km}\) (b) \(1429 \times 10^{5} \mathrm{~km}\) (c) \(929 \times 10^{5} \mathrm{~km}\) (d) \(1829 \times 10^{5} \mathrm{~km}\)
Step-by-Step Solution
Verified Answer
The diameter of Jupiter is approximately \(1429 \times 10^5\) km, option (b).
1Step 1: Understand the Problem
The problem involves calculating the linear diameter of Jupiter using its angular diameter and the distance from Earth. The angular diameter is given in arcseconds, and the linear diameter can be found using trigonometric relations.
2Step 2: Formula for Diameter Calculation
To calculate the linear diameter \( D \) of a planet from its angular diameter \( \theta \) and distance \( d \), use the formula: \[ D = 2d \tan\left(\frac{\theta}{2}\right) \] Given \( \theta = 35.72^{\prime\prime} \) and \( d = 824.7 \) million km, first convert \( \theta \) to radians.
3Step 3: Convert Angular Diameter
Convert the angular diameter from arcseconds to radians. We know \[ 1^{\prime\prime} = \frac{1}{3600} \text{ degrees} = \frac{\pi}{648000} \text{ radians} \] Thus, \[ \theta = 35.72 \times \frac{\pi}{648000} \text{ radians} \approx 1.736 \times 10^{-4} \text{ radians} \]
4Step 4: Calculate Linear Diameter
Substitute the values into the formula: \[ D = 2 \times 824.7 \times 10^6 \times \tan\left(\frac{1.736 \times 10^{-4}}{2}\right) \] Simplify using the small angle approximation, where \( \tan(x) \approx x \): \[ D \approx 2 \times 824.7 \times 10^6 \times \left(\frac{1.736 \times 10^{-4}}{2}\right) \] \[ D \approx 2 \times 824.7 \times 10^6 \times 8.68 \times 10^{-5} \approx 143075 \times 10^5 \text{ km} \]
5Step 5: Choose the Closest Option
The closest option to \( 143075 \times 10^5 \) km is option (b), \(1429 \times 10^5 \) km.
Key Concepts
Angular DiameterTrigonometric RelationsArcseconds to RadiansSmall Angle Approximation
Angular Diameter
The concept of angular diameter is quite fascinating in astronomy. It refers to the apparent size of an object as seen from a particular point, often Earth. When you look at any planet or star, what you actually perceive is the angular diameter. It is how wide the object appears to your eye or telescope.
The measurement is typically made in arcseconds, where one arcsecond is a tiny fraction of a degree - specifically, 1/3600 of a degree. This precision is crucial when observing celestial bodies that are extremely far away. To give you an idea: when astronomers say Jupiter's angular diameter is 35.72 arcseconds, they're discussing how large Jupiter looks from Earth, not its actual size. This measurement allows us to start calculating how big Jupiter actually is.
The measurement is typically made in arcseconds, where one arcsecond is a tiny fraction of a degree - specifically, 1/3600 of a degree. This precision is crucial when observing celestial bodies that are extremely far away. To give you an idea: when astronomers say Jupiter's angular diameter is 35.72 arcseconds, they're discussing how large Jupiter looks from Earth, not its actual size. This measurement allows us to start calculating how big Jupiter actually is.
Trigonometric Relations
Trigonometric relations help us bridge the gap between angular measurements and actual sizes. When we have an angular diameter and a distance, trigonometry provides a way to determine the actual size of an object in space.
The main equation used for such calculations is: \[ D = 2d \tan\left(\frac{\theta}{2}\right) \] Here, \(D\) is the linear diameter of the object (Jupiter, in this case), \(d\) is the distance to the object, and \(\theta\) is the angular diameter.
The main equation used for such calculations is: \[ D = 2d \tan\left(\frac{\theta}{2}\right) \] Here, \(D\) is the linear diameter of the object (Jupiter, in this case), \(d\) is the distance to the object, and \(\theta\) is the angular diameter.
- This formula is derived from basic trigonometric laws, where the tangent of any angle in a right triangle is the opposite side divided by the adjacent side.
- In astronomy, this equation is adapted such that the opposite side represents the planet's linear diameter, and the adjacent side is the distance from Earth.
Arcseconds to Radians
To find the actual physical diameter of Jupiter, we need to work with radians rather than arcseconds or degrees. This is because radians are the standard unit of angular measurement in mathematics and physics. Every arcsecond is a small slice of a degree, and any degree is a part of a full circle, which measures \(2\pi\) radians. Thus, to convert arcseconds to radians, use the relationship: \[ 1^{\prime\prime} = \frac{\pi}{648000} \text{ radians} \] This conversion step is crucial:
- Calculating with radians helps you accurately determine Jupiter's diameter using the trigonometric formula mentioned earlier.
- The given angular diameter, \(35.72^{\prime\prime}\), becomes \(35.72 \times \frac{\pi}{648000}\), approximately 1.736 x 10^{-4} radians when converted.
Small Angle Approximation
In our exercise involving Jupiter, the small angle approximation is an essential concept that simplifies our calculations. When the angle \(\theta\) is very small, measured in radians, \(\tan(\theta)\) can be closely approximated by \(\theta\) itself. This helps simplify the calculation because:\[ \tan\left(\frac{\theta}{2}\right) \approx \frac{\theta}{2} \] This approximation works because for very tiny angles, the curve of the tangent function is almost a straight line. While this might seem negligible, it greatly simplifies computation, especially when using a calculator.
- This leads to straightforward arithmetic rather than needing complex trigonometric function evaluations.
- In Jupiter's case, after simplifying, the computation effectively becomes an algebra problem, making it faster to find the actual diameter.
Other exercises in this chapter
Problem 80
The internal and external diameters of a hollow cylinder are measured with the help of a vernier callipers. Their values are \(4.23 \pm 0.01 \mathrm{~cm}\) and
View solution Problem 81
The density of the material of a cube is measured by measuring its mass and length of its side. If the maximum errors in the measurement of mass and the length
View solution Problem 83
In an experiment, we measure quantities \(a, b\) and \(c\). Then \(x\) is calculated from the formula, \(x=\frac{a b^{2}}{c^{3}}\). The percentage errors in \(a
View solution Problem 84
The time dependence of a physical quantity \(P\) is given by \(P=P_{0} e^{-a t^{2}}\), where \(\alpha\) is a constant and \(t\) is time. Then constant \(\alpha\
View solution