Conservation Law Fundamental Forces Estimation Of Distances L-2
CONSERVATION LAWS, FUNDAMENTAL FORCES, ESTIMATION OF DISTANCES
→ \rightarrow → → \rightarrow → CONSERVATION LAWS, FUNDAMENTAL FORCES, ESTIMATION OF DISTANCES → \rightarrow → Gravitation → \rightarrow → Work done
Conservation Law Fundamental Forces Estimation Of Distances L-2
Gravitation
It is assumed that the applied force is known.
Case of simple harmonic motion: F = − k x F=-k x F = − k x .
Case of electrostatic interaction: F = e 2 r 2 r ^ F=\frac{e^2}{r^2} \hat{r} F = r 2 e 2 r ^ = 1 e 1 e 2 4 π ϵ 0 r 2 r ^ \frac{1 e_1 e_2}{4 \pi \epsilon_0 r^2} \hat{r} 4 π ϵ 0 r 2 1 e 1 e 2 r ^
→ \rightarrow → CONSERVATION LAWS, FUNDAMENTAL FORCES, ESTIMATION OF DISTANCES → \rightarrow → Gravitation → \rightarrow → Work done → \rightarrow → Work done
Conservation Law Fundamental Forces Estimation Of Distances L-2
Work done
CONSERVATION LAWS, FUNDAMENTAL FORCES, ESTIMATION OF DISTANCES → \rightarrow → Gravitation → \rightarrow → Work done → \rightarrow → Work done → \rightarrow → Work done
Conservation Law Fundamental Forces Estimation Of Distances L-2
Work done
We say that a Force is Conservative, if the work done is independent of the path.
Gravitation → \rightarrow → Work done → \rightarrow → Work done → \rightarrow → Work done → \rightarrow → Work done
Conservation Law Fundamental Forces Estimation Of Distances L-2
Work done
Work done → \rightarrow → Work done → \rightarrow → Work done → \rightarrow → Work done → \rightarrow → Fundamental Forces
Conservation Law Fundamental Forces Estimation Of Distances L-2
Work done
F = − d V ( r ) d r F=-\frac{d V(r)}{d r} F = − d r d V ( r )
This is the statement of conservation of energy.
⇒ 1 2 m v ⃗ 2 + V ( r ) \Rightarrow \frac{1}{2} m \vec{v}^2+V(r) ⇒ 2 1 m v 2 + V ( r ) = Constant
1 2 m v ⃗ 2 \frac{1}{2} m \vec{v}^2 2 1 m v 2 = Kinetic Energy
V ( r ) V(r) V ( r ) = Potential Energy
Work done → \rightarrow → Work done → \rightarrow → Work done → \rightarrow → Fundamental Forces → \rightarrow → Fundamental Forces
Conservation Law Fundamental Forces Estimation Of Distances L-2
Fundamental Forces
Gravitation
Electromagnetic
Nuclear
Weak
Work done → \rightarrow → Work done → \rightarrow → Fundamental Forces → \rightarrow → Fundamental Forces → \rightarrow → Screening Effect
Conservation Law Fundamental Forces Estimation Of Distances L-2
Fundamental Forces
Interaction
Range
Strength
Gravitation
∞ \infty ∞
≈ 10 − 37 \approx 10^{-37} ≈ 1 0 − 37
Electromagnetic
∞ ( \infty( ∞ ( screened $)
≈ 10 − 2 \approx 10^{-2} ≈ 1 0 − 2
Nuclear Forces
10 − 15 m 10^{-15} \mathrm{~m} 1 0 − 15 m
≈ 1 \approx 1 ≈ 1
Weak Forces
< 10 − 17 m <10^{-17} \mathrm{~m} < 1 0 − 17 m
≈ 10 − 7 \approx 10^{-7} ≈ 1 0 − 7
Work done → \rightarrow → Fundamental Forces → \rightarrow → Fundamental Forces → \rightarrow → Screening Effect → \rightarrow → Nuclear Force
Conservation Law Fundamental Forces Estimation Of Distances L-2
Screening Effect
F G ∼ 1 r 2 F_G \sim \frac{1}{r^2} F G ∼ r 2 1
F E ∼ 1 r 2 F_E \sim \frac{1}{r^2} F E ∼ r 2 1
F E F_E F E can be positive and negative.
Every positive charge likes to get surrounded by negative charges vice-versa.
Because of this screening, the effective interaction between objects, is very weak compared to the gravitational force.
The range of electromagnetic forces become smaller.
Fundamental Forces → \rightarrow → Fundamental Forces → \rightarrow → Screening Effect → \rightarrow → Nuclear Force → \rightarrow → Gravitational Force
Conservation Law Fundamental Forces Estimation Of Distances L-2
Nuclear Force
Using Einstein's mass energy equivalents you can find how much energy is liberated in a nuclear reactor.
Fundamental Forces → \rightarrow → Screening Effect → \rightarrow → Nuclear Force → \rightarrow → Gravitational Force → \rightarrow → Universal Constant
Conservation Law Fundamental Forces Estimation Of Distances L-2
Gravitational Force
Screening Effect → \rightarrow → Nuclear Force → \rightarrow → Gravitational Force → \rightarrow → Universal Constant → \rightarrow → Distances and Masses
Conservation Law Fundamental Forces Estimation Of Distances L-2
Universal Constant
A particle of mass m is moving in the field of the sun's gravitational force.
Determine the universal constant.
m a = G M m r 2 ma = \frac{GMm}{r^2} ma = r 2 GM m
mass of A = m
mass of B = M
where, M >> m
Nuclear Force → \rightarrow → Gravitational Force → \rightarrow → Universal Constant → \rightarrow → Distances and Masses → \rightarrow → Radius of the Earth
Conservation Law Fundamental Forces Estimation Of Distances L-2
Distances and Masses
Size of the Earth
Size of the Moon
The Earth Moon distance
The Earth Sun distance
Masses of (i) The Earth, (ii) The Moon, and (iii) The stars
Gravitational Force → \rightarrow → Universal Constant → \rightarrow → Distances and Masses → \rightarrow → Radius of the Earth → \rightarrow → Radius of the Earth
Conservation Law Fundamental Forces Estimation Of Distances L-2
Radius of the Earth
Use trigonometry to find the radius of earth.
If we know the angle and distance, we should be able to estimate the radius of earth.
Universal Constant → \rightarrow → Distances and Masses → \rightarrow → Radius of the Earth → \rightarrow → Radius of the Earth → \rightarrow → Radius of the Earth Observation and Inference 4th Century BC
Conservation Law Fundamental Forces Estimation Of Distances L-2
Radius of the Earth
Distances and Masses → \rightarrow → Radius of the Earth → \rightarrow → Radius of the Earth → \rightarrow → Radius of the Earth Observation and Inference 4th Century BC → \rightarrow → Radius of the Earth
Conservation Law Fundamental Forces Estimation Of Distances L-2
Radius of the Earth Observation and Inference 4th Century BC
Eratosthenes found good methods of estimating the radius of the earth.
Radius of the Earth → \rightarrow → Radius of the Earth → \rightarrow → Radius of the Earth Observation and Inference 4th Century BC → \rightarrow → Radius of the Earth → \rightarrow → Earth-Moon Distance
Conservation Law Fundamental Forces Estimation Of Distances L-2
Radius of the Earth
Point corresponds to Alexandria.
Point corresponds to Aswan.
A well in Aswan and well contains water.
Distance between Alexandria and Aswan is known.
The distance is 50 stadium.
s = R θ s=R \theta s = Rθ
R = s θ R = \frac{s}{\theta} R = θ s = 800 km
C = 2 π R C = 2\pi R C = 2 π R = 40,000 km
Radius of the Earth → \rightarrow → Radius of the Earth Observation and Inference 4th Century BC → \rightarrow → Radius of the Earth → \rightarrow → Earth-Moon Distance → \rightarrow → Earth Sun and Moon Distance
Conservation Law Fundamental Forces Estimation Of Distances L-2
Earth-Moon Distance
Euclidean distance, not the shortest distance.
The sum of the angles of a triangle to be 180 degrees.
Radius of the Earth Observation and Inference 4th Century BC → \rightarrow → Radius of the Earth → \rightarrow → Earth-Moon Distance → \rightarrow → Earth Sun and Moon Distance → \rightarrow → Thank You
Conservation Law Fundamental Forces Estimation Of Distances L-2
Earth Sun and Moon Distance
The distance earth,moon and sun can find by trigonometry.
The new moon when the moon is completely on the opposite side of the earth.
The orbit of the moon is slightly inclined to this plane.
The moon would come between the earth and the sun. There would have been a solar eclipse.
Half moon is the eighth day, that day the moon is a perfect semicircle.
Radius of the Earth → \rightarrow → Earth-Moon Distance → \rightarrow → Earth Sun and Moon Distance → \rightarrow → Thank You → \rightarrow →
Conservation Law Fundamental Forces Estimation Of Distances L-2
Thank You
Earth-Moon Distance → \rightarrow → Earth Sun and Moon Distance → \rightarrow → Thank You → \rightarrow → → \rightarrow →
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Conservation Law Fundamental Forces Estimation Of Distances L-2 CONSERVATION LAWS, FUNDAMENTAL FORCES, ESTIMATION OF DISTANCES $\rightarrow$ $\rightarrow$ CONSERVATION LAWS, FUNDAMENTAL FORCES, ESTIMATION OF DISTANCES $\rightarrow$ Gravitation $\rightarrow$ Work done