What does the value of a probability density function (PDF) at some x indicate?












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I understand that the probability mass function of a discrete random-variable X is $y=g(x)$. This means $P(X=x_0) = g(x_0)$.



Now, a probability density function of of a continuous random variable X is $y=f(x)$. Wikipedia defines this function $y$ to mean




In probability theory, a probability density function (pdf), or density of a continuous random variable, is a function that describes the relative likelihood for this random variable to take on a given value.




I am confused about the meaning of 'relative likelihood' because it certainly does not mean probability! The probability $P(X<x_0)$ is given by some integral of the pdf.



So what does $f(x_0)$ indicate? It gives a real number, but isn't the relative likelihood of a specific value for a CRV always zero?










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  • 5




    $begingroup$
    Let $f$ be the density function of $X$. Assume $f$ is continuous. Then if $h$ is small, the probability that $X$ lies in the interval $[a,a+h]$ is approximately $hf(a)$. By approximately I mean that the probability, divided by $h$, approaches $f(a)$ as $h$ approaches $0$. So the ratio $f(a)/f(b)$ measures, approximately, the ratio of the probability that $X$ is in $[a,a+h]$ to the probability $X$ is in $[b,b+h]$.
    $endgroup$
    – André Nicolas
    Oct 10 '12 at 19:28
















10












$begingroup$


I understand that the probability mass function of a discrete random-variable X is $y=g(x)$. This means $P(X=x_0) = g(x_0)$.



Now, a probability density function of of a continuous random variable X is $y=f(x)$. Wikipedia defines this function $y$ to mean




In probability theory, a probability density function (pdf), or density of a continuous random variable, is a function that describes the relative likelihood for this random variable to take on a given value.




I am confused about the meaning of 'relative likelihood' because it certainly does not mean probability! The probability $P(X<x_0)$ is given by some integral of the pdf.



So what does $f(x_0)$ indicate? It gives a real number, but isn't the relative likelihood of a specific value for a CRV always zero?










share|cite|improve this question









$endgroup$








  • 5




    $begingroup$
    Let $f$ be the density function of $X$. Assume $f$ is continuous. Then if $h$ is small, the probability that $X$ lies in the interval $[a,a+h]$ is approximately $hf(a)$. By approximately I mean that the probability, divided by $h$, approaches $f(a)$ as $h$ approaches $0$. So the ratio $f(a)/f(b)$ measures, approximately, the ratio of the probability that $X$ is in $[a,a+h]$ to the probability $X$ is in $[b,b+h]$.
    $endgroup$
    – André Nicolas
    Oct 10 '12 at 19:28














10












10








10


7



$begingroup$


I understand that the probability mass function of a discrete random-variable X is $y=g(x)$. This means $P(X=x_0) = g(x_0)$.



Now, a probability density function of of a continuous random variable X is $y=f(x)$. Wikipedia defines this function $y$ to mean




In probability theory, a probability density function (pdf), or density of a continuous random variable, is a function that describes the relative likelihood for this random variable to take on a given value.




I am confused about the meaning of 'relative likelihood' because it certainly does not mean probability! The probability $P(X<x_0)$ is given by some integral of the pdf.



So what does $f(x_0)$ indicate? It gives a real number, but isn't the relative likelihood of a specific value for a CRV always zero?










share|cite|improve this question









$endgroup$




I understand that the probability mass function of a discrete random-variable X is $y=g(x)$. This means $P(X=x_0) = g(x_0)$.



Now, a probability density function of of a continuous random variable X is $y=f(x)$. Wikipedia defines this function $y$ to mean




In probability theory, a probability density function (pdf), or density of a continuous random variable, is a function that describes the relative likelihood for this random variable to take on a given value.




I am confused about the meaning of 'relative likelihood' because it certainly does not mean probability! The probability $P(X<x_0)$ is given by some integral of the pdf.



So what does $f(x_0)$ indicate? It gives a real number, but isn't the relative likelihood of a specific value for a CRV always zero?







probability statistics random-variables






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asked Oct 10 '12 at 19:20









jesterIIjesterII

1,20121326




1,20121326








  • 5




    $begingroup$
    Let $f$ be the density function of $X$. Assume $f$ is continuous. Then if $h$ is small, the probability that $X$ lies in the interval $[a,a+h]$ is approximately $hf(a)$. By approximately I mean that the probability, divided by $h$, approaches $f(a)$ as $h$ approaches $0$. So the ratio $f(a)/f(b)$ measures, approximately, the ratio of the probability that $X$ is in $[a,a+h]$ to the probability $X$ is in $[b,b+h]$.
    $endgroup$
    – André Nicolas
    Oct 10 '12 at 19:28














  • 5




    $begingroup$
    Let $f$ be the density function of $X$. Assume $f$ is continuous. Then if $h$ is small, the probability that $X$ lies in the interval $[a,a+h]$ is approximately $hf(a)$. By approximately I mean that the probability, divided by $h$, approaches $f(a)$ as $h$ approaches $0$. So the ratio $f(a)/f(b)$ measures, approximately, the ratio of the probability that $X$ is in $[a,a+h]$ to the probability $X$ is in $[b,b+h]$.
    $endgroup$
    – André Nicolas
    Oct 10 '12 at 19:28








5




5




$begingroup$
Let $f$ be the density function of $X$. Assume $f$ is continuous. Then if $h$ is small, the probability that $X$ lies in the interval $[a,a+h]$ is approximately $hf(a)$. By approximately I mean that the probability, divided by $h$, approaches $f(a)$ as $h$ approaches $0$. So the ratio $f(a)/f(b)$ measures, approximately, the ratio of the probability that $X$ is in $[a,a+h]$ to the probability $X$ is in $[b,b+h]$.
$endgroup$
– André Nicolas
Oct 10 '12 at 19:28




$begingroup$
Let $f$ be the density function of $X$. Assume $f$ is continuous. Then if $h$ is small, the probability that $X$ lies in the interval $[a,a+h]$ is approximately $hf(a)$. By approximately I mean that the probability, divided by $h$, approaches $f(a)$ as $h$ approaches $0$. So the ratio $f(a)/f(b)$ measures, approximately, the ratio of the probability that $X$ is in $[a,a+h]$ to the probability $X$ is in $[b,b+h]$.
$endgroup$
– André Nicolas
Oct 10 '12 at 19:28










5 Answers
5






active

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10












$begingroup$

'Relative likelihood' is indeed misleading. Look at it as a limit instead:
$$
f(x)=lim_{h to 0}frac{F(x+h)-F(x)}{h}
$$
where $F(x) = P(X leq x)$






share|cite|improve this answer









$endgroup$













  • $begingroup$
    So you suggest looking at the pdf as being defined by the cumulative distribution function?
    $endgroup$
    – jesterII
    Oct 10 '12 at 19:39








  • 2




    $begingroup$
    This is essentially the definition of pdf fro CRVs
    $endgroup$
    – Alex
    Oct 10 '12 at 20:12






  • 2




    $begingroup$
    A good way of thinking about is $f(x) = frac{dF}{dx}$ and so it's the rate of change of the cdf at $x$.
    $endgroup$
    – Jacob
    Feb 27 '13 at 17:39










  • $begingroup$
    Hi Alex, sorry for asking problem related to such an old answer. I know the pdf $f$ is the derivative of the cdf $F$, but what is the physical meaning of "the rate of change of the cdf at some point"? I mean, how to explain it by using the continuous random variable $X$?
    $endgroup$
    – Sam Wong
    Dec 13 '18 at 8:17












  • $begingroup$
    I don't know much about physics sorry.
    $endgroup$
    – Alex
    Dec 13 '18 at 10:55



















2












$begingroup$

In general, if $X$ is a random variable with values of a measure space $(A,mathcal A,mu)$ and with pdf $f:Ato [0,1]$, then for all measurable set $Sinmathcal A$,
$$P(Xin S) = int_S fdmu $$
So, if $A=Bbb R$ (and $mu=lambda$), then
$$P(a<X<b)=int_a^b f(x)dx$$
So, $f(x) = displaystylelim_{tto 0} frac1{2t}int_{x-t}^{x+t} f =lim_{tto 0} frac1{2t} P(|X-x|<t) $ for example.. We can call it 'relative likelihood'..






share|cite|improve this answer









$endgroup$









  • 1




    $begingroup$
    This is a better answer than Alex's but doesn't explain the significance of the number $f(x)$. Does it have a meaning independent of a cdf? Andre's answer of it being approximately $hf(a)$ is great but he doesn't indicate if there's more to $f(x)$ by itself.
    $endgroup$
    – Jacob
    Feb 27 '13 at 17:23





















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$begingroup$

Intro statistics focuses on the PDF as the description of the population, but in fact it is the CDF (cumulative density function) that gives you a functional understanding of the population, as points on the CDF denote probabilities over a relevant range of measures. If you look at all stats from this perspective, then the PDF is just the description of probability change with respect to a change around a point along the measure at hand. The values on the PDF therefore only give you a look at the spread. For example, given two normal distributions $N(mu_1, sigma_1^2)$ and $N(mu_2, sigma_2^2)$, if you choose any value of $x$ to get point $p_n=mu_n+xcdotsigma_n$ for the respective distributions and get $X_1[p_1 ] > X_2[p_2 ]$, then this just means $sigma_1 < sigma_2$. Similar relationships exist for other distributions.






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  • $begingroup$
    Very interesting answer!
    $endgroup$
    – information_interchange
    Jun 7 '18 at 18:38



















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I am not sure if Jester is still interested, as it's been 5 years, but I think I found a less confusing anwer than in Wikipedia.



In contrast to discrete random variables, if X is continuous, f(X) is a function whose value at any given sample is not the probability but rather it indicates the likelihood that X will be in that sample/interval. For example if the value of the PDF around a point (can be generalized for a sample) x is large, that means the random variable X is more likely to take values close to x. If, on the other hand, f(x)=0 in some interval, then X won't be in that interval



Of course a more practical way of thinking it is that the probability of X being in an interval is given by the integral of the PDF.



You might want to look at the link below for more details: http://mathinsight.org/probability_density_function_idea






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    0












    $begingroup$

    The ratio of the pdf $f(x)$ at two points, $r_x = f(x_0)/f(x_1)$, is not a measure of relative probability (or "relative likelihood") for the two outcomes for the random variable $X$. The ratio depends on the metric. That is, with a variable transformation, $z=z(x)$, with the pdf for $Z$ given by $h(z)$, the ratio $r_z=h(z_0)/h(z_1)neq r_x$, in general, even though the two ratios refer to the same two outcomes. For monotonic transformations, $f(x),dx = h(z),dz$.



    Numerical values of the pdf have no value on their own. The metric, $dx$, is required for probability interpretations (ie. $f(x),dx$). Wikipedia got this wrong, so I have corrected it.






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      5 Answers
      5






      active

      oldest

      votes








      5 Answers
      5






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes









      10












      $begingroup$

      'Relative likelihood' is indeed misleading. Look at it as a limit instead:
      $$
      f(x)=lim_{h to 0}frac{F(x+h)-F(x)}{h}
      $$
      where $F(x) = P(X leq x)$






      share|cite|improve this answer









      $endgroup$













      • $begingroup$
        So you suggest looking at the pdf as being defined by the cumulative distribution function?
        $endgroup$
        – jesterII
        Oct 10 '12 at 19:39








      • 2




        $begingroup$
        This is essentially the definition of pdf fro CRVs
        $endgroup$
        – Alex
        Oct 10 '12 at 20:12






      • 2




        $begingroup$
        A good way of thinking about is $f(x) = frac{dF}{dx}$ and so it's the rate of change of the cdf at $x$.
        $endgroup$
        – Jacob
        Feb 27 '13 at 17:39










      • $begingroup$
        Hi Alex, sorry for asking problem related to such an old answer. I know the pdf $f$ is the derivative of the cdf $F$, but what is the physical meaning of "the rate of change of the cdf at some point"? I mean, how to explain it by using the continuous random variable $X$?
        $endgroup$
        – Sam Wong
        Dec 13 '18 at 8:17












      • $begingroup$
        I don't know much about physics sorry.
        $endgroup$
        – Alex
        Dec 13 '18 at 10:55
















      10












      $begingroup$

      'Relative likelihood' is indeed misleading. Look at it as a limit instead:
      $$
      f(x)=lim_{h to 0}frac{F(x+h)-F(x)}{h}
      $$
      where $F(x) = P(X leq x)$






      share|cite|improve this answer









      $endgroup$













      • $begingroup$
        So you suggest looking at the pdf as being defined by the cumulative distribution function?
        $endgroup$
        – jesterII
        Oct 10 '12 at 19:39








      • 2




        $begingroup$
        This is essentially the definition of pdf fro CRVs
        $endgroup$
        – Alex
        Oct 10 '12 at 20:12






      • 2




        $begingroup$
        A good way of thinking about is $f(x) = frac{dF}{dx}$ and so it's the rate of change of the cdf at $x$.
        $endgroup$
        – Jacob
        Feb 27 '13 at 17:39










      • $begingroup$
        Hi Alex, sorry for asking problem related to such an old answer. I know the pdf $f$ is the derivative of the cdf $F$, but what is the physical meaning of "the rate of change of the cdf at some point"? I mean, how to explain it by using the continuous random variable $X$?
        $endgroup$
        – Sam Wong
        Dec 13 '18 at 8:17












      • $begingroup$
        I don't know much about physics sorry.
        $endgroup$
        – Alex
        Dec 13 '18 at 10:55














      10












      10








      10





      $begingroup$

      'Relative likelihood' is indeed misleading. Look at it as a limit instead:
      $$
      f(x)=lim_{h to 0}frac{F(x+h)-F(x)}{h}
      $$
      where $F(x) = P(X leq x)$






      share|cite|improve this answer









      $endgroup$



      'Relative likelihood' is indeed misleading. Look at it as a limit instead:
      $$
      f(x)=lim_{h to 0}frac{F(x+h)-F(x)}{h}
      $$
      where $F(x) = P(X leq x)$







      share|cite|improve this answer












      share|cite|improve this answer



      share|cite|improve this answer










      answered Oct 10 '12 at 19:28









      AlexAlex

      14.2k42134




      14.2k42134












      • $begingroup$
        So you suggest looking at the pdf as being defined by the cumulative distribution function?
        $endgroup$
        – jesterII
        Oct 10 '12 at 19:39








      • 2




        $begingroup$
        This is essentially the definition of pdf fro CRVs
        $endgroup$
        – Alex
        Oct 10 '12 at 20:12






      • 2




        $begingroup$
        A good way of thinking about is $f(x) = frac{dF}{dx}$ and so it's the rate of change of the cdf at $x$.
        $endgroup$
        – Jacob
        Feb 27 '13 at 17:39










      • $begingroup$
        Hi Alex, sorry for asking problem related to such an old answer. I know the pdf $f$ is the derivative of the cdf $F$, but what is the physical meaning of "the rate of change of the cdf at some point"? I mean, how to explain it by using the continuous random variable $X$?
        $endgroup$
        – Sam Wong
        Dec 13 '18 at 8:17












      • $begingroup$
        I don't know much about physics sorry.
        $endgroup$
        – Alex
        Dec 13 '18 at 10:55


















      • $begingroup$
        So you suggest looking at the pdf as being defined by the cumulative distribution function?
        $endgroup$
        – jesterII
        Oct 10 '12 at 19:39








      • 2




        $begingroup$
        This is essentially the definition of pdf fro CRVs
        $endgroup$
        – Alex
        Oct 10 '12 at 20:12






      • 2




        $begingroup$
        A good way of thinking about is $f(x) = frac{dF}{dx}$ and so it's the rate of change of the cdf at $x$.
        $endgroup$
        – Jacob
        Feb 27 '13 at 17:39










      • $begingroup$
        Hi Alex, sorry for asking problem related to such an old answer. I know the pdf $f$ is the derivative of the cdf $F$, but what is the physical meaning of "the rate of change of the cdf at some point"? I mean, how to explain it by using the continuous random variable $X$?
        $endgroup$
        – Sam Wong
        Dec 13 '18 at 8:17












      • $begingroup$
        I don't know much about physics sorry.
        $endgroup$
        – Alex
        Dec 13 '18 at 10:55
















      $begingroup$
      So you suggest looking at the pdf as being defined by the cumulative distribution function?
      $endgroup$
      – jesterII
      Oct 10 '12 at 19:39






      $begingroup$
      So you suggest looking at the pdf as being defined by the cumulative distribution function?
      $endgroup$
      – jesterII
      Oct 10 '12 at 19:39






      2




      2




      $begingroup$
      This is essentially the definition of pdf fro CRVs
      $endgroup$
      – Alex
      Oct 10 '12 at 20:12




      $begingroup$
      This is essentially the definition of pdf fro CRVs
      $endgroup$
      – Alex
      Oct 10 '12 at 20:12




      2




      2




      $begingroup$
      A good way of thinking about is $f(x) = frac{dF}{dx}$ and so it's the rate of change of the cdf at $x$.
      $endgroup$
      – Jacob
      Feb 27 '13 at 17:39




      $begingroup$
      A good way of thinking about is $f(x) = frac{dF}{dx}$ and so it's the rate of change of the cdf at $x$.
      $endgroup$
      – Jacob
      Feb 27 '13 at 17:39












      $begingroup$
      Hi Alex, sorry for asking problem related to such an old answer. I know the pdf $f$ is the derivative of the cdf $F$, but what is the physical meaning of "the rate of change of the cdf at some point"? I mean, how to explain it by using the continuous random variable $X$?
      $endgroup$
      – Sam Wong
      Dec 13 '18 at 8:17






      $begingroup$
      Hi Alex, sorry for asking problem related to such an old answer. I know the pdf $f$ is the derivative of the cdf $F$, but what is the physical meaning of "the rate of change of the cdf at some point"? I mean, how to explain it by using the continuous random variable $X$?
      $endgroup$
      – Sam Wong
      Dec 13 '18 at 8:17














      $begingroup$
      I don't know much about physics sorry.
      $endgroup$
      – Alex
      Dec 13 '18 at 10:55




      $begingroup$
      I don't know much about physics sorry.
      $endgroup$
      – Alex
      Dec 13 '18 at 10:55











      2












      $begingroup$

      In general, if $X$ is a random variable with values of a measure space $(A,mathcal A,mu)$ and with pdf $f:Ato [0,1]$, then for all measurable set $Sinmathcal A$,
      $$P(Xin S) = int_S fdmu $$
      So, if $A=Bbb R$ (and $mu=lambda$), then
      $$P(a<X<b)=int_a^b f(x)dx$$
      So, $f(x) = displaystylelim_{tto 0} frac1{2t}int_{x-t}^{x+t} f =lim_{tto 0} frac1{2t} P(|X-x|<t) $ for example.. We can call it 'relative likelihood'..






      share|cite|improve this answer









      $endgroup$









      • 1




        $begingroup$
        This is a better answer than Alex's but doesn't explain the significance of the number $f(x)$. Does it have a meaning independent of a cdf? Andre's answer of it being approximately $hf(a)$ is great but he doesn't indicate if there's more to $f(x)$ by itself.
        $endgroup$
        – Jacob
        Feb 27 '13 at 17:23


















      2












      $begingroup$

      In general, if $X$ is a random variable with values of a measure space $(A,mathcal A,mu)$ and with pdf $f:Ato [0,1]$, then for all measurable set $Sinmathcal A$,
      $$P(Xin S) = int_S fdmu $$
      So, if $A=Bbb R$ (and $mu=lambda$), then
      $$P(a<X<b)=int_a^b f(x)dx$$
      So, $f(x) = displaystylelim_{tto 0} frac1{2t}int_{x-t}^{x+t} f =lim_{tto 0} frac1{2t} P(|X-x|<t) $ for example.. We can call it 'relative likelihood'..






      share|cite|improve this answer









      $endgroup$









      • 1




        $begingroup$
        This is a better answer than Alex's but doesn't explain the significance of the number $f(x)$. Does it have a meaning independent of a cdf? Andre's answer of it being approximately $hf(a)$ is great but he doesn't indicate if there's more to $f(x)$ by itself.
        $endgroup$
        – Jacob
        Feb 27 '13 at 17:23
















      2












      2








      2





      $begingroup$

      In general, if $X$ is a random variable with values of a measure space $(A,mathcal A,mu)$ and with pdf $f:Ato [0,1]$, then for all measurable set $Sinmathcal A$,
      $$P(Xin S) = int_S fdmu $$
      So, if $A=Bbb R$ (and $mu=lambda$), then
      $$P(a<X<b)=int_a^b f(x)dx$$
      So, $f(x) = displaystylelim_{tto 0} frac1{2t}int_{x-t}^{x+t} f =lim_{tto 0} frac1{2t} P(|X-x|<t) $ for example.. We can call it 'relative likelihood'..






      share|cite|improve this answer









      $endgroup$



      In general, if $X$ is a random variable with values of a measure space $(A,mathcal A,mu)$ and with pdf $f:Ato [0,1]$, then for all measurable set $Sinmathcal A$,
      $$P(Xin S) = int_S fdmu $$
      So, if $A=Bbb R$ (and $mu=lambda$), then
      $$P(a<X<b)=int_a^b f(x)dx$$
      So, $f(x) = displaystylelim_{tto 0} frac1{2t}int_{x-t}^{x+t} f =lim_{tto 0} frac1{2t} P(|X-x|<t) $ for example.. We can call it 'relative likelihood'..







      share|cite|improve this answer












      share|cite|improve this answer



      share|cite|improve this answer










      answered Oct 10 '12 at 19:30









      BerciBerci

      60k23672




      60k23672








      • 1




        $begingroup$
        This is a better answer than Alex's but doesn't explain the significance of the number $f(x)$. Does it have a meaning independent of a cdf? Andre's answer of it being approximately $hf(a)$ is great but he doesn't indicate if there's more to $f(x)$ by itself.
        $endgroup$
        – Jacob
        Feb 27 '13 at 17:23
















      • 1




        $begingroup$
        This is a better answer than Alex's but doesn't explain the significance of the number $f(x)$. Does it have a meaning independent of a cdf? Andre's answer of it being approximately $hf(a)$ is great but he doesn't indicate if there's more to $f(x)$ by itself.
        $endgroup$
        – Jacob
        Feb 27 '13 at 17:23










      1




      1




      $begingroup$
      This is a better answer than Alex's but doesn't explain the significance of the number $f(x)$. Does it have a meaning independent of a cdf? Andre's answer of it being approximately $hf(a)$ is great but he doesn't indicate if there's more to $f(x)$ by itself.
      $endgroup$
      – Jacob
      Feb 27 '13 at 17:23






      $begingroup$
      This is a better answer than Alex's but doesn't explain the significance of the number $f(x)$. Does it have a meaning independent of a cdf? Andre's answer of it being approximately $hf(a)$ is great but he doesn't indicate if there's more to $f(x)$ by itself.
      $endgroup$
      – Jacob
      Feb 27 '13 at 17:23













      2












      $begingroup$

      Intro statistics focuses on the PDF as the description of the population, but in fact it is the CDF (cumulative density function) that gives you a functional understanding of the population, as points on the CDF denote probabilities over a relevant range of measures. If you look at all stats from this perspective, then the PDF is just the description of probability change with respect to a change around a point along the measure at hand. The values on the PDF therefore only give you a look at the spread. For example, given two normal distributions $N(mu_1, sigma_1^2)$ and $N(mu_2, sigma_2^2)$, if you choose any value of $x$ to get point $p_n=mu_n+xcdotsigma_n$ for the respective distributions and get $X_1[p_1 ] > X_2[p_2 ]$, then this just means $sigma_1 < sigma_2$. Similar relationships exist for other distributions.






      share|cite|improve this answer









      $endgroup$













      • $begingroup$
        Very interesting answer!
        $endgroup$
        – information_interchange
        Jun 7 '18 at 18:38
















      2












      $begingroup$

      Intro statistics focuses on the PDF as the description of the population, but in fact it is the CDF (cumulative density function) that gives you a functional understanding of the population, as points on the CDF denote probabilities over a relevant range of measures. If you look at all stats from this perspective, then the PDF is just the description of probability change with respect to a change around a point along the measure at hand. The values on the PDF therefore only give you a look at the spread. For example, given two normal distributions $N(mu_1, sigma_1^2)$ and $N(mu_2, sigma_2^2)$, if you choose any value of $x$ to get point $p_n=mu_n+xcdotsigma_n$ for the respective distributions and get $X_1[p_1 ] > X_2[p_2 ]$, then this just means $sigma_1 < sigma_2$. Similar relationships exist for other distributions.






      share|cite|improve this answer









      $endgroup$













      • $begingroup$
        Very interesting answer!
        $endgroup$
        – information_interchange
        Jun 7 '18 at 18:38














      2












      2








      2





      $begingroup$

      Intro statistics focuses on the PDF as the description of the population, but in fact it is the CDF (cumulative density function) that gives you a functional understanding of the population, as points on the CDF denote probabilities over a relevant range of measures. If you look at all stats from this perspective, then the PDF is just the description of probability change with respect to a change around a point along the measure at hand. The values on the PDF therefore only give you a look at the spread. For example, given two normal distributions $N(mu_1, sigma_1^2)$ and $N(mu_2, sigma_2^2)$, if you choose any value of $x$ to get point $p_n=mu_n+xcdotsigma_n$ for the respective distributions and get $X_1[p_1 ] > X_2[p_2 ]$, then this just means $sigma_1 < sigma_2$. Similar relationships exist for other distributions.






      share|cite|improve this answer









      $endgroup$



      Intro statistics focuses on the PDF as the description of the population, but in fact it is the CDF (cumulative density function) that gives you a functional understanding of the population, as points on the CDF denote probabilities over a relevant range of measures. If you look at all stats from this perspective, then the PDF is just the description of probability change with respect to a change around a point along the measure at hand. The values on the PDF therefore only give you a look at the spread. For example, given two normal distributions $N(mu_1, sigma_1^2)$ and $N(mu_2, sigma_2^2)$, if you choose any value of $x$ to get point $p_n=mu_n+xcdotsigma_n$ for the respective distributions and get $X_1[p_1 ] > X_2[p_2 ]$, then this just means $sigma_1 < sigma_2$. Similar relationships exist for other distributions.







      share|cite|improve this answer












      share|cite|improve this answer



      share|cite|improve this answer










      answered Jun 28 '15 at 14:44









      TopherTopher

      347317




      347317












      • $begingroup$
        Very interesting answer!
        $endgroup$
        – information_interchange
        Jun 7 '18 at 18:38


















      • $begingroup$
        Very interesting answer!
        $endgroup$
        – information_interchange
        Jun 7 '18 at 18:38
















      $begingroup$
      Very interesting answer!
      $endgroup$
      – information_interchange
      Jun 7 '18 at 18:38




      $begingroup$
      Very interesting answer!
      $endgroup$
      – information_interchange
      Jun 7 '18 at 18:38











      2












      $begingroup$

      I am not sure if Jester is still interested, as it's been 5 years, but I think I found a less confusing anwer than in Wikipedia.



      In contrast to discrete random variables, if X is continuous, f(X) is a function whose value at any given sample is not the probability but rather it indicates the likelihood that X will be in that sample/interval. For example if the value of the PDF around a point (can be generalized for a sample) x is large, that means the random variable X is more likely to take values close to x. If, on the other hand, f(x)=0 in some interval, then X won't be in that interval



      Of course a more practical way of thinking it is that the probability of X being in an interval is given by the integral of the PDF.



      You might want to look at the link below for more details: http://mathinsight.org/probability_density_function_idea






      share|cite|improve this answer









      $endgroup$


















        2












        $begingroup$

        I am not sure if Jester is still interested, as it's been 5 years, but I think I found a less confusing anwer than in Wikipedia.



        In contrast to discrete random variables, if X is continuous, f(X) is a function whose value at any given sample is not the probability but rather it indicates the likelihood that X will be in that sample/interval. For example if the value of the PDF around a point (can be generalized for a sample) x is large, that means the random variable X is more likely to take values close to x. If, on the other hand, f(x)=0 in some interval, then X won't be in that interval



        Of course a more practical way of thinking it is that the probability of X being in an interval is given by the integral of the PDF.



        You might want to look at the link below for more details: http://mathinsight.org/probability_density_function_idea






        share|cite|improve this answer









        $endgroup$
















          2












          2








          2





          $begingroup$

          I am not sure if Jester is still interested, as it's been 5 years, but I think I found a less confusing anwer than in Wikipedia.



          In contrast to discrete random variables, if X is continuous, f(X) is a function whose value at any given sample is not the probability but rather it indicates the likelihood that X will be in that sample/interval. For example if the value of the PDF around a point (can be generalized for a sample) x is large, that means the random variable X is more likely to take values close to x. If, on the other hand, f(x)=0 in some interval, then X won't be in that interval



          Of course a more practical way of thinking it is that the probability of X being in an interval is given by the integral of the PDF.



          You might want to look at the link below for more details: http://mathinsight.org/probability_density_function_idea






          share|cite|improve this answer









          $endgroup$



          I am not sure if Jester is still interested, as it's been 5 years, but I think I found a less confusing anwer than in Wikipedia.



          In contrast to discrete random variables, if X is continuous, f(X) is a function whose value at any given sample is not the probability but rather it indicates the likelihood that X will be in that sample/interval. For example if the value of the PDF around a point (can be generalized for a sample) x is large, that means the random variable X is more likely to take values close to x. If, on the other hand, f(x)=0 in some interval, then X won't be in that interval



          Of course a more practical way of thinking it is that the probability of X being in an interval is given by the integral of the PDF.



          You might want to look at the link below for more details: http://mathinsight.org/probability_density_function_idea







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Oct 24 '17 at 23:25









          ALEX.VAMVASALEX.VAMVAS

          211




          211























              0












              $begingroup$

              The ratio of the pdf $f(x)$ at two points, $r_x = f(x_0)/f(x_1)$, is not a measure of relative probability (or "relative likelihood") for the two outcomes for the random variable $X$. The ratio depends on the metric. That is, with a variable transformation, $z=z(x)$, with the pdf for $Z$ given by $h(z)$, the ratio $r_z=h(z_0)/h(z_1)neq r_x$, in general, even though the two ratios refer to the same two outcomes. For monotonic transformations, $f(x),dx = h(z),dz$.



              Numerical values of the pdf have no value on their own. The metric, $dx$, is required for probability interpretations (ie. $f(x),dx$). Wikipedia got this wrong, so I have corrected it.






              share|cite|improve this answer









              $endgroup$


















                0












                $begingroup$

                The ratio of the pdf $f(x)$ at two points, $r_x = f(x_0)/f(x_1)$, is not a measure of relative probability (or "relative likelihood") for the two outcomes for the random variable $X$. The ratio depends on the metric. That is, with a variable transformation, $z=z(x)$, with the pdf for $Z$ given by $h(z)$, the ratio $r_z=h(z_0)/h(z_1)neq r_x$, in general, even though the two ratios refer to the same two outcomes. For monotonic transformations, $f(x),dx = h(z),dz$.



                Numerical values of the pdf have no value on their own. The metric, $dx$, is required for probability interpretations (ie. $f(x),dx$). Wikipedia got this wrong, so I have corrected it.






                share|cite|improve this answer









                $endgroup$
















                  0












                  0








                  0





                  $begingroup$

                  The ratio of the pdf $f(x)$ at two points, $r_x = f(x_0)/f(x_1)$, is not a measure of relative probability (or "relative likelihood") for the two outcomes for the random variable $X$. The ratio depends on the metric. That is, with a variable transformation, $z=z(x)$, with the pdf for $Z$ given by $h(z)$, the ratio $r_z=h(z_0)/h(z_1)neq r_x$, in general, even though the two ratios refer to the same two outcomes. For monotonic transformations, $f(x),dx = h(z),dz$.



                  Numerical values of the pdf have no value on their own. The metric, $dx$, is required for probability interpretations (ie. $f(x),dx$). Wikipedia got this wrong, so I have corrected it.






                  share|cite|improve this answer









                  $endgroup$



                  The ratio of the pdf $f(x)$ at two points, $r_x = f(x_0)/f(x_1)$, is not a measure of relative probability (or "relative likelihood") for the two outcomes for the random variable $X$. The ratio depends on the metric. That is, with a variable transformation, $z=z(x)$, with the pdf for $Z$ given by $h(z)$, the ratio $r_z=h(z_0)/h(z_1)neq r_x$, in general, even though the two ratios refer to the same two outcomes. For monotonic transformations, $f(x),dx = h(z),dz$.



                  Numerical values of the pdf have no value on their own. The metric, $dx$, is required for probability interpretations (ie. $f(x),dx$). Wikipedia got this wrong, so I have corrected it.







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered Nov 27 '16 at 0:47









                  DeanDean

                  1,00537




                  1,00537






























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