

How Laplace Correction Improves Probability Estimates in Physics
Laplace Correction gives correction to the speed of sound in the gas. The formula for the speed of sound in the gaseous medium was estimated by Newton, he assumed that the propagation of sound waves in air or gas is under isothermal condition. This assumption was found contradictory, the speed of sound in the air was found to be 280m/s which wasn’t accurate. Thus, Laplace came up with a correction to it which was evident theoretically as well as practically. Thus it is well known as a Laplace Correction to Newton’s Formula.
What is Laplace Correction?
Laplace corrected that- the propagation of sound waves takes place under adiabatic conditions. The thermal conductivity of air is so less than the movement of compression and rarefaction in the air will be rapid, resulting in that the heat flows neither out of the system nor into the system, i.e., the change in heat applied will be zero, which is clearly an adiabatic condition. This is known as Laplace Correction for sound waves in air or gaseous medium. The sound speed of a gas is corrected using Laplace Correction. Laplace devised a theoretical as well as a practical adjustment. As a result, Newton's Formula is usually referred to as a Laplace adjustment.
Laplace Correction for Newton’s Formula:
According to the theory of Newton, the compression and rarefaction in the air is an isothermal process and the speed of sound is given by:
v=Pρ−−√≈280m/sv=Pρ≈280m/s
Where,
P - Pressure in the medium
ρ - Medium density
We know that the speed of sound in the air medium is around 332m/s. The value obtained by Newton’s formula was 280m/s which is not accurate. To overcome this difficulty, Laplace conducted a few experiments and came up with a correction and hence derived Laplace Correction Formula.
Laplace carried out the same approach of Newton with a modification that the compression and rarefaction in the air is an adiabatic process as the thermal conductivity in the air will be very less and rapid. He assumed that the compression and rarefaction are completely insulated adiabatic processes, that the change in heat applied will be zero or constant.
Laplace Correction Derivation:
Since we are assuming that the compression and rarefaction are adiabatic processes, then the gas equation for the adiabatic process is given by:
⇒PVγ = Constant………(1)Where,
P
P - Pressure in the medium
V - Volume of the gas
γ - Adiabatic index
Now, differentiate equation (1) on both sides,
⇒γPVγ−1dV+VγdP=0
⇒γPVγ−1dV+VγdP=0⇒Vγ−1
[γPdV+VdP]=0⇒Vγ−1[γPdV+VdP]=0⇒γPdv+Vdp=0
⇒γPdv+Vdp=0 On rearranging the above equation,
⇒γPdV=−VdP⇒γPdV=−VdP⇒γP=−PDV⇒γP=−VdPdV……..(2)−VdPdV
−VdPdV is−√v=γPρ…….(5) ium
ρ - Medium density
γ - Adiabatic index
Equation (5) is known as the Laplace Correction for speed of sound or the Laplace formula for the speed of sound. The Laplace Correction in Physics is in good agreement with the value of the speed of sound in the air at standard pressure and temperature.
Example:
1. Calculate the Speed of Sound Using Laplace Correction and Newton’s Formula at Standard Pressure and Temperature. Compare the Values.
Ans:
i) The velocity of sound by Laplace Correction formula is given by:
\[\Rightarrow v=\sqrt{\frac{\gamma p}{\rho }}\]
Where,
P - Pressure in the medium=1.101×105N/m2
ρ = Medium density=1.293Kg/m3
ρ - Adiabatic index=1.4
Substituting the corresponding values in the equation,
\[\Rightarrow v=\sqrt{\frac{1.4\times 1.101\times10^{5} }{1.293}}=345m/s\approx 332m/s\]
ii) The velocity of sound by Newton’s formula is given by:
\[\Rightarrow v=\sqrt{\frac{p}{\rho }}\]
where,
P - Pressure in the medium=1.101×105N/m2
ρ - Medium density =1.293kg/m3
Substituting the values in the equation,
\[\Rightarrow v=\sqrt{\frac{1.101\times10^{5} }{1.293}}=290m/s\]
By comparing the values of speed of sound by Laplace Correction and Newton’s formula, it is evident that the value obtained with the Laplace Correction formula is in good agreement with the value of sound in air in comparison to the value obtained by Newton’s formula. Hence it is known as Laplace Correction to Newton’s formula.
Things to Keep in Mind about Laplace Correction
When sound waves travel through the air, compression and rarefaction occur, according to Newton. Furthermore, the processes are quite slow.
According to Laplace, the compression and rarefaction processes occur relatively quickly with little heat exchange.
Sound wave velocities: The two qualities of matter that determine the velocity of sound are inertia and elasticity. The velocity of sound has been calculated in a medium with elasticity E and density.
A denser medium is determined by a lower velocity, and vice versa. As a result, when sound travels from air to water, it bends away from its regular path. The sound beam of light, on the other hand, bends towards the normal.
When sound travels through air, according to Newton, the temperature remains constant (i.e. the process is isothermal).
Why choose Vedantu?
Vedantu is a web-based platform that provides free PDF downloads and quick access to all problem-solving resources. The topics presented in the school curriculum are simply downloaded and read by students. They also provide online instruction for the students studying for the entrance examinations like NEET and JEE. All of the lecturers are professionals in their professions and can help students plan for the future. You may also use the website to study for board examinations and admissions exams. All the topics are explained in detail and the experts make sure that they use easy and simple language while explaining the topics so that it becomes easy for the students to understand, learn and study. We have a specialized and professional team of experts who work hard for preparing the solutions and notes for students. We want every student to score by studying from our solutions which are available for free and in PDF format. It can be downloaded for offline use.
FAQs on Laplace Correction: Concept, Formula & Applications
1. What is Laplace's correction in the context of sound waves?
Laplace's correction is a modification to Newton's original formula for the speed of sound in a gas. Laplace proposed that the propagation of sound is not an isothermal process (constant temperature) as Newton assumed, but an adiabatic process (no heat exchange). This correction accounts for the temperature changes that occur in the regions of compression and rarefaction, leading to a more accurate calculation of the speed of sound.
2. Why was Newton's formula for the speed of sound incorrect?
Newton's formula was found to be incorrect because it underestimated the speed of sound in air by about 16%. The discrepancy arose from a flawed assumption. Newton assumed that the compressions and rarefactions caused by a sound wave occur so slowly that heat has enough time to flow between them, keeping the temperature constant (an isothermal process). However, sound waves travel too quickly for this heat exchange to happen, which is why Laplace's adiabatic assumption was necessary.
3. What is the formula for the speed of sound according to Laplace's correction?
The formula for the speed of sound (v) in a gas, as corrected by Laplace, is given by:
v = √(γP/ρ)
Where:
- γ (gamma) is the adiabatic index or ratio of specific heats (Cp/Cv).
- P is the pressure of the gas.
- ρ (rho) is the density of the gas.
4. How does the adiabatic process assumption lead to a more accurate value for the speed of sound?
The assumption of an adiabatic process acknowledges that sound waves create very rapid compressions and rarefactions.
- In compressions, air particles are pushed together, increasing the temperature.
- In rarefactions, particles move apart, decreasing the temperature.
5. What is the importance of the adiabatic index (γ) in Laplace's correction?
The adiabatic index (γ) is crucial because it represents the ratio of the specific heat of a gas at constant pressure to its specific heat at constant volume (Cp/Cv). It quantifies how much the temperature of a gas changes during an adiabatic compression or expansion. For air (which is mostly diatomic), the value of γ is approximately 1.4. Multiplying the pressure (P) by γ in the formula effectively increases the bulk modulus of the gas, accounting for the additional pressure changes due to temperature fluctuations, which Newton's formula ignored.
6. How are compressions and rarefactions defined in a sound wave?
In a longitudinal wave like sound, compressions and rarefactions describe the density of the medium's particles:
- Compression: This is a region where the particles of the medium are crowded together, resulting in a momentary increase in density and pressure.
- Rarefaction: This is a region where the particles are spread far apart, resulting in a momentary decrease in density and pressure.
7. What is the practical application of Laplace's corrected formula?
The primary application of Laplace's corrected formula is to accurately calculate the speed of sound in various gaseous media. This is fundamental in many fields, including:
- Acoustics: For designing concert halls, speakers, and sound-related equipment.
- Meteorology: To understand atmospheric phenomena and in technologies like SODAR (sonic detection and ranging).
- Physics and Engineering: For calibrating instruments, studying material properties, and in fluid dynamics research.
8. Can Laplace's correction be applied to sound travelling through liquids or solids?
While the concept of adiabatic compression is relevant, the specific formula v = √(γP/ρ) is derived for gases. For liquids and solids, the speed of sound is determined by their elastic properties, specifically the Bulk Modulus (B) for liquids and Young's Modulus (Y) for solids. The formulas are different:
- For liquids: v = √(B/ρ)
- For solids (in a thin rod): v = √(Y/ρ)





















